SCI-ext Makaleler

2018  (161 Yayın)

 

Alevli, M. and N. Gungor (2018). "Influence of N-2/H-2 and N-2 plasma on binary III-nitride films prepared by hollow-cathode plasma-assisted atomic layer deposition." Journal of Vacuum Science & Technology A 36(1).
   
Baltaci, H., Akkoyunlu, B.O., et al. (2018). "An Extreme Hailstorm on 27 July 2017 in Istanbul, Turkey: Synoptic Scale Circulation and Thermodynamic Evaluation." Pure and Applied Geophysics 175(11): 3727-3740.
   
Baltaci, H., Akkoyunlu, B.O., et al. (2018). "Relationships between teleconnection patterns and Turkish climatic extremes." Theoretical and Applied Climatology 134(3-4): 1365-1386.
   
Coskun, M., Dumludag, F., et al. (2018). "Bridged oxide nanowire device fabrication using single step metal catalyst free thermal evaporation." Rsc Advances 8(19): 10294-10301.
   
Dumludag, F., et al. (2018). DC and AC conductivity properties of bovine dentine hydroxyapatite (BDHA). 3rd International Conference on Smart Material Research. 293.
   
Dumludag, F., et al. (2018). Effects of sintering temperature on electrical properties of sheep enamel hydroxyapatite. 3rd International Conference on Smart Material Research. 293.
   
Ghasemifard, M., Okay, C., et al. (2018). "Bond length (Ti-O) dependence of nano ATO(3)-based (A = Pb, Ba, Sr) perovskite structures: Optical investigation in IR range." Modern Physics Letters B 32(1).
   
Gungor, N. and M. Alevli (2018). "Role of film thickness on the structural and optical properties of GaN on Si (100) grown by hollow-cathode plasma-assisted atomic layer deposition." Journal of Vacuum Science & Technology A 36(2).
   
Inanc, A., Kosoglu, C., et al. (2018). "3-D optical profilometry at micron scale with multi-frequency fringe projection using modified fibre optic Lloyd's mirror technique." Optics and Lasers in Engineering 105: 14-26.
   
Koksoy, B., Dumludag, F., et al. (2018). "Electrical and gas sensing properties of novel cobalt(II), copper(II), manganese(III) phthalocyanines carrying ethyl 7-oxy-4,8-dimethylcoumarin-3-propanoate moieties." Journal of Porphyrins and Phthalocyanines 22(1-3): 121-136.
   
Liu, T. D., Altun, Z., et al. (2018). "Phosphorescence Tuning through Heavy Atom Placement in Unsymmetrical Difluoroboron beta-Diketonate Materials." Chemistry-a European Journal 24(8): 1859-1869.
   
Okay, C., Deger, C., et al. (2018). "Tailoring the magnetic anisotropy of cobalt-gold thin films." Turkish Journal of Physics 42(3): 335-341.
   
Ozer, H. and O. Delice (2018). "Linearized modified gravity theories with a cosmological term: advance of perihelion and deflection of light." Classical and Quantum Gravity 35(6).
   
Sirunyan, A. M., et al. (2018). "Measurement of b hadron lifetimes in pp collisions at root s=8TeV." European Physical Journal C 78(6).
   
Sirunyan, A. M., et al. (2018). "Search for Heavy Neutral Leptons in Events with Three Charged Leptons in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 120(22).
   
Sirunyan, A. M., et al. (2018). "Search for Leptoquarks Coupled to Third-Generation Quarks in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 121(24).
   
Sirunyan, A. M., et al. (2018). "Search for Pair-Produced Resonances Each Decaying into at Least Four Quarks in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 121(14).
   
Sirunyan, A. M., et al. (2018). "Search for new physics in events with a leptonically decaying Z boson and a large transverse momentum imbalance in proton-proton collisions at root s=13 TeV." European Physical Journal C 78(4).
   
Sirunyan, A. M., et al. (2018). "Search for the X(5568) State Decaying into B-s(0)pi(+/-) in Proton-Proton Collisions at root s=8 TeV." Physical Review Letters 120(20).
   
Sirunyan, A. M., et al. (2018). "Search for supersymmetry in proton-proton collisions at 13 TeV using identified top quarks." Physical Review D 97(1).
   
Sirunyan, A. M., et al. (2018). "Search for natural and split supersymmetry in proton-proton collisions at root s=13 TeV in final states with jets and missing transverse momentum." Journal of High Energy Physics(5).
   
Sirunyan, A. M., et al. (2018). "Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state root s=13 TeV." Journal of High Energy Physics(5).
   
Sirunyan, A. M., et al. (2018). "Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at root s(NN)=5.02 TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Electroweak production of two jets in association with a Z boson in proton-proton collisions root s =13 TeV." European Physical Journal C 78(7).
   
Sirunyan, A. M., et al. (2018). "Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying tau leptons at root s=13 TeV." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Evidence for the Higgs boson decay to a bottom quark-antiquark pair." Physics Letters B 780: 501-532.
   
Sirunyan, A. M., et al. (2018). "Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV." Journal of Instrumentation 13.
   
Sirunyan, A. M., et al. (2018). "Measurement of the associated production of a single top quark and a Z boson in pp collisions at, root s=13 TeV." Physics Letters B 779: 358-384.
   
Sirunyan, A. M., et al. (2018). "Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Measurement of the Lambda(b) polarization and angular parameters in Lambda(b) -> J/psi Lambda decays from pp collisions at root s=7 and 8 TeV." Physical Review D 97(7).
   
Sirunyan, A. M., et al. (2018). "Measurement of the Z/gamma* -> tau tau cross section in pp collisions at root s=13 TeV and validation of tau lepton analysis techniques." European Physical Journal C 78(9).
   
Sirunyan, A. M., et al. (2018). "Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Observation of Medium-Induced Modifications of Jet Fragmentation in Pb-Pb Collisions at root s(NN)=5.02 TeV Using Isolated Photon-Tagged Jets." Physical Review Letters 121(24).
   
Sirunyan, A. M., et al. (2018). "Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at root s=13 TeV." Journal of Instrumentation 13.
   
Sirunyan, A. M., et al. (2018). "Search for a heavy resonance decaying into a Z boson and a vector boson in the v(v)over-barq(q)over-bar final state." Journal of High Energy Physics(7).
   
Sirunyan, A. M., et al. (2018). "Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2l2q final states at root s=13 TeV." Journal of High Energy Physics(9).
   
Sirunyan, A. M., et al. (2018). "Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets root s at=13 TeV." Journal of High Energy Physics(5).
   
Sirunyan, A. M., et al. (2018). "Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for additional neutral MSSM Higgs bosons in the tau tau final state in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(9).
   
Sirunyan, A. M., et al. (2018). "Search for high-mass resonances in dilepton final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for lepton-flavor violating decays of heavy resonances and quantum black holes to e mu final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(4).
   
Sirunyan, A. M., et al. (2018). "Search for narrow and broad dijet resonances in proton-proton collisions at root s=13 TeV and constraints on dark matter mediators and other new particles." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Search for Narrow Resonances in the b-Tagged Dijet Mass Spectrum in Proton-Proton Collisions at root s=8 TeV." Physical Review Letters 120(20).
   
Sirunyan, A. M., et al. (2018). "Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models." European Physical Journal C 78(9).
   
Sirunyan, A. M., et al. (2018). "Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at root s=13 TeV." Physics Letters B 782: 440-467.
   
Sirunyan, A. M., et al. (2018). "Search for new physics in final states with an energetic jet or a hadronically decaying W or Z boson and transverse momentum imbalance at root s=13 TeV." Physical Review D 97(9).
   
Sirunyan, A. M., et al. (2018). "Search for pair production of excited top quarks in the lepton plus jets final state The CMS Collaboration." Physics Letters B 778: 349-370.
   
Sirunyan, A. M., et al. (2018). "Search for Physics Beyond the Standard Model in Events with High-Momentum Higgs Bosons and Missing Transverse Momentum in Proton-Proton Collisions at 13 TeV." Physical Review Letters 120(24).
   
Sirunyan, A. M., et al. (2018). "Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Search for R-parity violating supersymmetry in pp collisions at root s=13 TeV using bjets in a final state with a single lepton, many jets, and high sum of large-radius jet masses." Physics Letters B 783: 114-139.
   
Sirunyan, A. M., et al. (2018). "Search for single production of vector-like quarks decaying to a b quark and a Higgs boson." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for standard model production of four top quarks with same-sign and multilepton final states in proton-proton collisions at root s=13TeV." European Physical Journal C 78(2).
   
Sirunyan, A. M., et al. (2018). "Search for t(t)over-barH production in the all-jet final state in proton-proton collisions root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for third-generation scalar leptoquarks decaying to a top quark and a tau lepton at root s=13 TeV." European Physical Journal C 78(9).
   
Sirunyan, A. M., et al. (2018). "Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(9).
   
Sirunyan, A. M., et al. (2018). "Search for ZZ resonances in the 2l2v final state in proton-proton collisions at 13 TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Jet properties in PbPb and pp collisions at root S-NN=5.02 TeV." Journal of High Energy Physics(5).
   
Sirunyan, A. M., et al. (2018). "Measurement of differential cross sections for the production of top quark pairs and of additional jets in lepton plus jets events from pp collisions at root s=13 TeV." Physical Review D 97(11).
   
Sirunyan, A. M., et al. (2018). "Measurement of differential cross sections for Z boson production in association with jets in proton- proton collisions at v s=13TeV." European Physical Journal C 78(11).
   
Sirunyan, A. M., et al. (2018). "Measurement of the inelastic proton-proton cross section at root s=13 TeV." Journal of High Energy Physics(7).
   
Sirunyan, A. M., et al. (2018). "Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer." Journal of High Energy Physics(7).
   
Sirunyan, A. M., et al. (2018). "Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(10).
   
Sirunyan, A. M., et al. (2018). "Precision measurement of the structure of the CMS inner tracking system using nuclear interactions." Journal of Instrumentation 13.
   
Sirunyan, A. M., et al. (2018). "Angular analysis of the decay B+ -> K+mu(+)mu(-) in proton-proton collisions at root s=8 TeV." Physical Review D 98(11).
   
Sirunyan, A. M., et al. (2018). "Elliptic Flow of Charm and Strange Hadrons in High-Multiplicity p plus Pb Collisions at root(NN)-N-s=8.16 TeV." Physical Review Letters 121(8).
   
Sirunyan, A. M., et al. (2018). "Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV." European Physical Journal C 78(9).
   
Sirunyan, A. M., et al. (2018). "Measurement of jet substructure observables in t(t)over-bar events from proton-proton collisions at root s=13 TeV." Physical Review D 98(9).
   
Sirunyan, A. M., et al. (2018). "Measurement of the weak mixing angle using the forward-backward asymmetry of Drell-Yan events in pp collisions at 8 TeV." European Physical Journal C 78(9).
   
Sirunyan, A. M., et al. (2018). "Observation of the Z -> psi l(+)l(-) Decay in pp Collisions at root s=13 TeV." Physical Review Letters 121(14).
   
Sirunyan, A. M., et al. (2018). "Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at root s=8TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration." Physics Letters B 785: 462-488.
   
Sirunyan, A. M., et al. (2018). "Search for beyond the standard model Higgs bosons decaying into a b(b)over-bar pair in pp collisions at root s=13 TeV." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at root s=13 TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Search for supersymmetry in events with a tau lepton pair and missing transverse momentum in proton-proton collisions at root s=13TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Search for the decay of a Higgs boson in the ll gamma channel in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(9).
   
Sirunyan, A. M., et al. (2018). "Search for vector-like T and B quark pairs in final states with leptons at root s=13 TeV." Journal of High Energy Physics(8).
   
Sirunyan, A. M., et al. (2018). "Observation of Electroweak Production of Same-Sign W Boson Pairs in the Two Jet and Two Same-Sign Lepton Final State in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 120(8).
   
Sirunyan, A. M., et al. (2018). "Measurements of the pp -> ZZ production cross section and the Z -> 4l branching fraction, and constraints on anomalous triple gauge couplings at root s=13TeV." European Physical Journal C 78(2).
   
Sirunyan, A. M., et al. (2018). "Measurement of associated Z plus charm production in proton-proton collisions at root s=8TeV." European Physical Journal C 78(4).
   
Sirunyan, A. M., et al. (2018). "Pseudorapidity and transverse momentum dependence of flow harmonics in pPb and PbPb collisions." Physical Review C 98(4).
   
Sirunyan, A. M., et al. (2018). "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at root s=13 TeV." European Physical Journal C 78(7).
   
Sirunyan, A. M., et al. (2018). "Bose-Einstein correlations in pp, pPb, and PbPb collisions at root s(NN)=0.9-7 TeV." Physical Review C 97(6).
   
Sirunyan, A. M., et al. (2018). "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the CERN Large Hadron Collider." Physical Review C 97(4).
   
Sirunyan, A. M., et al. (2018). "Constraintson the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at root s=8TeV." Journal of High Energy Physics(2).
   
Sirunyan, A. M., et al. (2018). "Inclusive Search for a Highly Boosted Higgs Boson Decaying to a Bottom Quark-Antiquark Pair." Physical Review Letters 120(7).
   
Sirunyan, A. M., et al. (2018). "Measurement of angular parameters from the decay B-0 -> K*(0)mu(+)mu(-) in proton-proton collisions at root s=8 TeV." Physics Letters B 781: 517-541.
   
Sirunyan, A. M., et al. (2018). "Measurement of b hadron lifetimes in pp collisions at root s = 8TeV (vol 78, 2018)." European Physical Journal C 78(7).
   
Sirunyan, A. M., et al. (2018). "Measurement of differential cross sections in the kinematic angular variable phi* for inclusive Z boson production in pp collisions at root s=8 TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Measurement of normalized differential t(t)over-bar cross sections in the dilepton channel from pp collisions at root s=13 TeV." Journal of High Energy Physics(4).
   
Sirunyan, A. M., et al. (2018). "Measurement of prompt and nonprompt charmonium suppression in PbPb collisions at 5.02 TeV." European Physical Journal C 78(6).
   
Sirunyan, A. M., et al. (2018). "Measurement of Prompt D-0 Meson Azimuthal Anisotropy in Pb-Pb Collisions at root S-NN=5.02 TeV." Physical Review Letters 120(20).
   
Sirunyan, A. M., et al. (2018). "Measurement of quarkonium production cross sections in pp collisions at root s=13 TeV." Physics Letters B 780: 251-272.
   
Sirunyan, A. M., et al. (2018). "Measurement of the Splitting Function in &ITpp &ITand Pb-Pb Collisions at root&ITsNN&IT=5.02 TeV." Physical Review Letters 120(14).
   
Sirunyan, A. M., et al. (2018). "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(7).
   
Sirunyan, A. M., et al. (2018). "Measurements of the pp -> ZZ production cross section and the Z -> 4l branching fraction, and constraints on anomalous triple gauge couplings at root s = 13 TeV (vol 78, 165, 2018)." European Physical Journal C 78(6).
   
Sirunyan, A. M., et al. (2018). "Nuclear modification factor of D-0 mesons in PbPb collisions at root s(NN)=5.02 TeV." Physics Letters B 782: 474-496.
   
Sirunyan, A. M., et al. (2018). "Observation of Correlated Azimuthal Anisotropy Fourier Harmonics in pp and p plus Pb Collisions at the LHC." Physical Review Letters 120(9).
   
Sirunyan, A. M., et al. (2018). "Observation of the Higgs boson decay to a pair of tau leptons with the CMS detector." Physics Letters B 779: 283-316.
   
Sirunyan, A. M., et al. (2018). "Search for a massive resonance decaying to a pair of Higgs bosons in the four b quark final state in proton-proton collisions at root s=13 TeV." Physics Letters B 781: 244-269.
   
Sirunyan, A. M., et al. (2018). "Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Search for excited quarks of light and heavy flavor in gamma plus jet final states in proton-proton collisions at root s=13 TeV." Physics Letters B 781: 390-411.
   
Sirunyan, A. M., et al. (2018). "Search for gauge-mediated supersymmetry in events with at least one photon and missing transverse momentum in pp collisions at ,root s=13 TeV." Physics Letters B 780: 118-143.
   
Sirunyan, A. M., et al. (2018). "Search for heavy resonances decaying to a top quark and a bottom quark in the lepton plus jets final state in proton-proton collisions at 13 TeV." Physics Letters B 777: 39-63.
   
Sirunyan, A. M., et al. (2018). "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at root s=13 TeV." Physics Letters B 778: 101-127.
   
Sirunyan, A. M., et al. (2018). "Search for Higgsino pair production in pp collisions at root s=13 TeV in final states with large missing transverse momentum and two Higgs bosons decaying via H -> b(b)over bar." Physical Review D 97(3).
   
Sirunyan, A. M., et al. (2018). "Search for lepton flavour violating decays of the Higgs boson to mu tau and e tau in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
   
Sirunyan, A. M., et al. (2018). "Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(1).
   
Sirunyan, A. M., et al. (2018). "Search for massive resonances decaying into WW, WZ, ZZ, qW, and qZ with dijet final states at root s=13 TeV." Physical Review D 97(7).
   
Sirunyan, A. M., et al. (2018). "Search for new long-lived particles at root s=13 TeV." Physics Letters B 780: 432-454.
   
Sirunyan, A. M., et al. (2018). "Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at root s=13TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Search for pair production of vector-like quarks in the bW(b)over-barW channel from proton-proton collisions at root s=13TeV." Physics Letters B 779: 82-106.
   
Sirunyan, A. M., et al. (2018). "Search for resonant and nonresonant Higgs boson pair production in the b(b)over-barl nu l nu final state in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(1).
   
Sirunyan, A. M., et al. (2018). "Search for single production of a vector- like T quark decaying to a Z boson and a top quark in proton-proton collisions at root s=13 TeV." Physics Letters B 781: 574-600.
   
Sirunyan, A. M., et al. (2018). "Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(2).
   
Sirunyan, A. M., et al. (2018). "Search for supersymmetry in events with one lepton and multiple jets exploiting the angular correlation between the lepton and the missing transverse momentum in proton-proton collisions at root s=13 TeV." Physics Letters B 780: 384-409.
   
Sirunyan, A. M., et al. (2018). "Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at root s=13 TeV." Physics Letters B 779: 166-190.
   
Sirunyan, A. M., et al. (2018). "Search for the pair production of third-generation squarks with two-body decays to a bottom or charm quark and a neutralino in proton-proton collisions at root s=13 TeV." Physics Letters B 778: 263-291.
   
Sirunyan, A. M., et al. (2018). "Study of jet quenching with isolated-photon plus jet correlations in PbPb and pp collisions at root s(NN)=5.02 TeV." Physics Letters B 785: 14-39.
   
Sirunyan, A. M., et al. (2018). "Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Measurement of the inclusive t(t)over-bar cross section in pp collisions root s=5.02 TeV using final states with at least one charged lepton." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Search for top squarks and dark matter particles in opposite-charge dilepton final states at root s=13 TeV." Physical Review D 97(3).
   
Sirunyan, A. M., et al. (2018). "Pseudorapidity distributions of charged hadrons in proton-lead collisions at root s(NN)=5:02 and 8.16 TeV." Journal of High Energy Physics(1).
   
Sirunyan, A. M., et al. (2018). "Evidence for the Associated Production of a Single Top Quark and a Photon in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 121(22).
   
Sirunyan, A. M., et al. (2018). "Performance of reconstruction and identification of tau leptons decaying to hadrons and nu(tau) in pp collisions at root s=13 TeV." Journal of Instrumentation 13.
   
Sirunyan, A. M., et al. (2018). "Charged-particle nuclear modification factors in XeXe collisions at root S-NN=5.44 TeV." Journal of High Energy Physics(10).
   
Sirunyan, A. M., et al. (2018). "Constraining Gluon Distributions in Nuclei Using Dijets in Proton-Proton and Proton-Lead Collisions at root s(NN)=5.02 TeV." Physical Review Letters 121(6).
   
Sirunyan, A. M., et al. (2018). "Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at root s=13 TeV." Physical Review D 98(3).
   
Sirunyan, A. M., et al. (2018). "Event shape variables measured using multijet final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(12).
   
Sirunyan, A. M., et al. (2018). "Measurement of the groomed jet mass in PbPb and pp collisions at root s(NN)=5:02 TeV." Journal of High Energy Physics(10).
   
Sirunyan, A. M., et al. (2018). "Measurement of the top quark mass with lepton plus jets final states using pp collisions at root s=13 TeV." European Physical Journal C 78(11).
   
Sirunyan, A. M., et al. (2018). "Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton -proton collisions at=13 TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Observation of (tt)over-barH Production." Physical Review Letters 120(23).
   
Sirunyan, A. M., et al. (2018). "Observation of Higgs Boson Decay to Bottom Quarks." Physical Review Letters 121(12).
   
Sirunyan, A. M., et al. (2018). "Observation of the chi(b1)(3P) and chi(b2)(3P) and Measurement of their Masses." Physical Review Letters 121(9).
   
Sirunyan, A. M., et al. (2018). "Search for a singly produced third-generation scalar leptoquark decaying to a tau lepton and a bottom quark in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(7).
   
Sirunyan, A. M., et al. (2018). "Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two tau leptons in proton-proton collisions at TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions a root s=13 TeVt." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Search for dark matter produced in association with a Higgs boson decaying to gamma gamma or tau(+)tau(-) at root s=13 TeV." Journal of High Energy Physics(9).
   
Sirunyan, A. M., et al. (2018). "Search for long-lived particles with displaced vertices in multijet events in proton-proton collisions at root s=13 TeV." Physical Review D 98(9).
   
Sirunyan, A. M., et al. (2018). "Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at root s=13 TeV." Physical Review D 98(11).
   
Sirunyan, A. M., et al. (2018). "Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at root s=13 TeV." Physical Review D 98(9).
   
Sirunyan, A. M., et al. (2018). "Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at root 8 and 13 TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
   
Sirunyan, A. M., et al. (2018). "Studies of B-s2*(5840)(0) and B-s1(5830)(0) mesons including the observation of the B-s2*(5840)(0) -> (BKS0)-K-0 decay in proton- proton collisions at root s=8 TeV." European Physical Journal C 78(11).
   
Sirunyan, A. M., et al. (2018). "Azimuthal anisotropy of charged particles with transverse momentum up to 100GeV/c in PbPb collisions at root S-NN=5.02 TeV." Physics Letters B 776: 195-216.
   
Sirunyan, A. M., et al. (2018). "Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at root s = 13 TeV (vol 9, 106, 2017)." Journal of High Energy Physics(1).
   
Sirunyan, A. M., et al. (2018). "Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at root s=8 TeV." Journal of High Energy Physics(3).
   
Sirunyan, A. M., et al. (2018). "Search for vectorlike light-flavor quark partners in proton-proton collisions at root s=8 TeV." Physical Review D 97(7).
   
Sirunyan, A. M., et al. (2018). "Study of dijet events with a large rapidity gap between the two leading jets in pp collisions at root s=7 TeV." European Physical Journal C 78(3).
   
Sirunyan, A. M., et al. (2018). "Suppression of Excited gamma States Relative to the Ground State in Pb-Pb Collisions at root s(NN)=5.02 TeV." Physical Review Letters 120(14).
   
Sirunyan, A. M., et al. (2018). "Measurements of t(t)over-bar cross sections in association with b jets and inclusive jets and their ratio using dilepton final states in pp collisions at root s=13 TeV." Physics Letters B 776: 355-378.
   
Tabanli, S., Erdem, M., et al. (2018). "Broadband, White Light Emission from Doped and Undoped Insulators." Ecs Journal of Solid State Science and Technology 7(1): R3199-R3210.
   
Ulutas, K., Yahsi, U.,et al. (2018). "Dielectric properties and conductivity of PVdF-co-HFP/LiClO4 polymer electrolytes." Canadian Journal of Physics 96(7): 786-791.
   
Yabas, E., Dumludag, F., et al. (2018). "Imidazole octasubstituted novel mono and double-decker phthalocyanines: Synthesis, characterization, electrical and gas sensing properties." Polyhedron 153: 51-63.
   
Yavuz, I., Altun, Z., et al. (2018). "Control of molecular dissociation by spatially inhomogeneous near fields." Physical Review A 98(4).
   


2017  (126 Yayın)

 

Altun, Z., Bleda, E., et al. (2017). "Single metal catalysis: DFT and CAS modelling of species involved in the Fe cation assisted transformation of acetylene to benzene." Molecular Physics 115(17-18): 2185-2200.
  
Cinkaya, H., Erdem, M., et al. (2017). Investigation of the Luminescence Spectral Profiles and the Efficiencies of Yb3+, Nd3+, Tm3+ Doped Y2O3-SiO2 Nano-phosphors. Nano-Optics: Principles Enabling Basic Research and Applications. B. DiBartolo, J. Collins and L. Silvestri: 441-444.
    
Cinkaya, H., Erdem, M., et al. (2017). "Effect of pressure and temperature on the white light produed by Ytterbium (III) doped and undoped Yttrium Silicate nanopowders excited by a laser diode." Journal of Luminescence 181: 321-326.
    
Erkan, K., Akkoyunlu, B., et al. (2017). "A portable borehole temperature logging system using the four-wire resistance method." Journal of Geophysics and Engineering 14(6): 1413-1419.
    
Kalayci, T., Deger, C., et al. (2017). "Tuning magnetic properties of non-collinear magnetization configuration in Pt/ Pt/Co (6)/Pt/Co/Pt multilayer structure." Journal of magnetism and magnetic materials 436: 11-16.
    
Khachatryan, V., et al. (2017). "Measurement of differential cross sections for top quark pair production using the lepton plus jets final state in proton-proton collisions at 13 TeV." Physical Review D 95(9).
    
Khachatryan, V., et al. (2017). "Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at root s=13 TeV." Physical Review D 95(1).
    
Khachatryan, V., et al. (2017). "Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at root S-NN=2.76 TeV." European Physical Journal C 77(4).
    
Khachatryan, V., et al. (2017). "Measurements of the associated production of a Z boson and b jets in pp collisions at root s=8 TeV." European Physical Journal C 77(11).
    
Khachatryan, V., et al. (2017). "Measurement of the differential inclusive B+ hadron cross sections in pp collisions at root s=13TeV." Physics Letters B 771: 435-456.
    
Khachatryan, V., et al. (2017). "Measurement of the t(t)over-bar production cross section using events in the e mu final state in pp collisions at root s=13 TeV." European Physical Journal C 77(3).
    
Khachatryan, V., et al. (2017). "search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jet (vol 12, 083, 2016)." Journal of High Energy Physics(8).
    
Khachatryan, V., et al. (2017). "The CMS trigger system." Journal of Instrumentation 12.
    
Khachatryan, V., et al. (2017). "Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV." Journal of Instrumentation 12.
    
Khachatryan, V., et al. (2017). "Measurements of the t(t)over-bar production cross section in lepton plus jets final states in pp collisions at 8 and ratio of 8 to 7 cross sections." European Physical Journal C 77(1): 1-27.
    
Khachatryan, V., et al. (2017). "Pseudorapidity dependence of long-range two-particle correlations in pPb collisions at root sNN=5.02 TeV." Physical Review C 96(1).
    
Khachatryan, V., et al. (2017). "Coherent J/psi photoproduction in ultra-peripheral PbPb collisions at root s(NN)=2.76 TeV with the CMS experiment." Physics Letters B 772: 489-511.
    
Khachatryan, V., et al. (2017). "Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at root s=8TeV." Journal of High Energy Physics(2).
    
Khachatryan, V., et al. (2017). "Multiplicity and rapidity dependence of strange hadron production in pp, pPb, and PbPb collisions at the LHC." Physics Letters B 768: 103-129.
    
Khachatryan, V., et al. (2017). "Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at root s=8 TeV using the alpha(T) variable." Physics Letters B 767: 403-430.
    
Khachatryan, V., et al. (2017). "Charged-particle nuclear modification factors in PbPb and pPb collisions at root s(NN)=5.02 TeV." Journal of High Energy Physics(4).
    
Khachatryan, V., et al. (2017). "Evidence for collectivity in pp collisions at the LHC." Physics Letters B 765: 193-220.
    
Khachatryan, V., et al. (2017). "Inclusive search for supersymmetry using razor variables in pp collisions at root s=13 TeV." Physical Review D 95(1).
    
Khachatryan, V., et al. (2017). "Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at root s=8 TeV and cross section ratios to 2.76 and 7 TeV." Journal of High Energy Physics(3).
    
Khachatryan, V., et al. (2017). "Measurement of electroweak-induced production of W gamma with two jets in pp collisions at root s=8TeV and constraints on anomalous quartic gauge couplings." Journal of High Energy Physics(6).
    
Khachatryan, V., et al. (2017). "Measurement of inclusive jet cross sections in pp and PbPb collisions at root s(NN)=2.76 TeV." Physical Review C 96(1).
    
Khachatryan, V., et al. (2017). "Measurement of the cross section for electroweak production of Z gamma in association with two jets and constraints on anomalous quartic gauge couplings in proton-proton collisions at root s=8 TeV." Physics Letters B 770: 380-402.
    
Khachatryan, V., et al. (2017). "Measurement of the production cross section of a W boson in association with two b jets in pp collisions at root s=8TeV." European Physical Journal C 77(2).
    
Khachatryan, V., et al. (2017). "Measurement of the WZ production cross section in pp collisions at root s=7 and 8 TeV and search for anomalous triple gauge couplings at root s=8 TeV." European Physical Journal C 77(4).
    
Khachatryan, V., et al. (2017). "Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at root s=8 TeV." Physical Review D 95(5).
    
Khachatryan, V., et al. (2017). "Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at root s=8 TeV." Journal of High Energy Physics(4).
    
Khachatryan, V., et al. (2017). "Observation of Charge-Dependent Azimuthal Correlations in p-Pb Collisions and Its Implication for the Search for the Chiral Magnetic Effect." Physical Review Letters 118(12).
    
Khachatryan, V., et al. (2017). "Observation of gamma(1S) pair production in proton-proton collisions at root s=8 TeV." Journal of High Energy Physics(5).
    
Khachatryan, V., et al. (2017). "Observation of the decay B+ -> psi(2S)phi(1020)K+ in pp collisions at root s=8 TeV." Physics Letters B 764: 66-86.
    
Khachatryan, V., et al. (2017). "Search for anomalous Wtb couplings and flavour-changing neutral currents in t-channel single top quark production in pp collisions at root s=7 and 8 TeV." Journal of High Energy Physics(2).
    
Khachatryan, V., et al. (2017). "Search for CP violation in t(t)over-bar production and decay in proton-proton collisions at root s=8 TeV." Journal of High Energy Physics(3).
    
Khachatryan, V., et al. (2017). "Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV." Physical Review Letters 118(2).
    
Khachatryan, V., et al. (2017). "Search for electroweak production of charginos in final states with two T leptons in pp collisions at root s=8 TeV." Journal of High Energy Physics(4).
    
Khachatryan, V., et al. (2017). "Search for heavy gauge W ' bosons in events with an energetic lepton and large missing transverse momentum at root s=13TeV." Physics Letters B 770: 278-301.
    
Khachatryan, V., et al. (2017). "Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying tau leptons and two jets in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
    
Khachatryan, V., et al. (2017). "Search for high-mass diphoton resonances in proton-proton collisions at 13 TeV and combination with 8 TeV search." Physics Letters B 767: 147-170.
    
Khachatryan, V., et al. (2017). "Search for high-mass Z gamma resonances in e(+)e(-)gamma and mu(+)mu(-)gamma final states in proton-proton collisions at root s=8 and 13 TeV." Journal of High Energy Physics(1).
    
Khachatryan, V., et al. (2017). "Search for leptophobic Z ' bosons decaying into four-lepton final states in proton-proton collisions at root s=8 TeV." Physics Letters B 773: 563-584.
    
Khachatryan, V., et al. (2017). "Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at root s=8 TeV." Journal of High Energy Physics(10).
    
Khachatryan, V., et al. (2017). "Search for narrow resonances in dilepton mass spectra in proton-proton collisions at root s=13 TeV and combination with 8 TeV data." Physics Letters B 768: 57-80.
    
Khachatryan, V., et al. (2017). "A search for new phenomena in pp collisions at root s=13TeV in final states with missing transverse momentum and at least one jet using the alpha(T) variable." European Physical Journal C 77(5).
    
Khachatryan, V., et al. (2017). "Search for R-parity violating supersymmetry with displaced vertices in proton-proton collisions at root s=8 TeV." Physical Review D 95(1).
    
Khachatryan, V., et al. (2017). "Search for single production of a heavy vector-like T quark decaying to a Higgs boson and a top quark with a lepton and jets in the final state." Physics Letters B 771: 80-105.
    
Khachatryan, V., et al. (2017). "Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at root s=8 TeV." Journal of High Energy Physics(2).
    
Khachatryan, V., et al. (2017). "Searches for invisible decays of the Higgs boson in pp collisions at root S=7, 8, and 13 TeV." Journal of High Energy Physics(2).
    
Khachatryan, V., et al. (2017). "Suppression of gamma(1S), gamma(2S), and gamma(3S) quarkonium states in PbPb collisions at root S-NN=2.76TeV." Physics Letters B 770: 357-379.
    
Khachatryan, V., et al. (2017). "Search for supersymmetry in events with photons and missing transverse energy in pp collisions at 13 TeV." Physics Letters B 769: 391-412.
    
Khachatryan, V., et al. (2017). "Search for new phenomena with multiple charged leptons in proton-proton collisions at root s=13TeV." European Physical Journal C 77(9).
    
Khachatryan, V., et al. (2017). "Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at root s=13 TeV." Physical Review D 96(1).
    
Kirezli, P. and O. Delice (2017). Some Properties of Magnetized Bonnor-Dihole Solution in Brans-Dicke Theory. Proceedings of the Turkish Physical Society 32nd International Physics Congress. B. Akkus, Y. Oktem, G. S. Dogan and F. Guzelcimen. 1815.
    
Sertkol, M., et al. (2017). "Thermoelectric and Magnetic Properties of Pt-Substituted BaFe4-xPtxSb12 Compounds." Journal of Electronic Materials 46(1): 73-78.
    
Sirunyan, A. M., et al. (2017). "Constraints on anomalous Higgs boson couplings using production and decay information in the four-lepton final state." Physics Letters B 775: 1-24.
    
Sirunyan, A. M., et al. (2017). "Measurement of the top quark mass in the dileptonic t(t)over-bar decay channel using the mass observables M-bl, M-T2, and M-blv in pp collisions at root=8 TeV." Physical Review D 96(3).
    
Sirunyan, A. M., et al. (2017). "Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at root s=13TeV." European Physical Journal C 77(9).
    
Sirunyan, A. M., et al. (2017). "Search for Supersymmetry in pp Collisions at root s=13 TeV in the Single-Lepton Final State Using the Sum of Masses of Large-Radius Jets." Physical Review Letters 119(15).
    
Sirunyan, A. M., et al. (2017). "Search for a heavy composite Majorana neutrino in the final state with two leptons and two quarks at root s=13 TeV." Physics Letters B 775: 315-337.
    
Sirunyan, A. M., et al. (2017). "Searches for W ' bosons decaying to a top quark and a bottom quark in proton-proton collisions at 13TeV." Journal of High Energy Physics(8): 1-42.
    
Sirunyan, A. M., et al. (2017). "Measurement of the differential cross sections for the associated production of a W boson and jets in proton-proton collisions at root s=13 TeV." Physical Review D 96(7).
    
Sirunyan, A. M., et al. (2017). "Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton-proton collisions at root s=13 TeV." Physics Letters B 774: 682-705.
    
Sirunyan, A. M., et al. (2017). "Principal-component analysis of two-particle azimuthal correlations in PbPb and pPb collisions at CMS." Physical Review C 96(6).
    
Sirunyan, A. M., et al. (2017). "Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at root s=8 TeV." Journal of High Energy Physics(11).
    
Sirunyan, A. M., et al. (2017). "Search for direct production of super symmetric partners of the top quark in the all-jets final state in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Search for electroweak production of charginos and neutralinos in WH events in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
    
Sirunyan, A. M., et al. (2017). "Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 119(22).
    
Sirunyan, A. M., et al. (2017). "Search for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton-proton collisions at root s=13TeV." European Physical Journal C 77(9).
    
Sirunyan, A. M., et al. (2017). "Search for supersymmetry in events with at least one photon, missing transverse momentum, and large transverse event activity in proton-proton collisions at root s=13TeV." Journal of High Energy Physics(12).
    
Sirunyan, A. M., et al. (2017). "Search for supersymmetry in multijet events with missing transverse momentum in proton-proton collisions at 13 TeV." Physical Review D 96(3).
    
Sirunyan, A. M., et al. (2017). "Search for top squark pair production in pp collisions at root s=13 TeV using single lepton events." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
    
Sirunyan, A. M., et al. (2017). "Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at root s=13 TeV." Journal of High Energy Physics(11).
    
Sirunyan, A. M., et al. (2017). "Search for standard model production of four top quarks in proton-proton collisions at root s=13TeV." Physics Letters B 772: 336-358.
    
Sirunyan, A. M., et al. (2017). "Measurement of prompt and nonprompt J/psi production in pp and pPb collisions at root s(NN)=5.02 TeV." European Physical Journal C 77(4).
    
Sirunyan, A. M., et al. (2017). "Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton-proton collisions at root s=8 and 13 TeV." Physics Letters B 774: 533-558.
    
Sirunyan, A. M., et al. (2017). "Cross section measurement of t-channel single top quark production in pp collisions at root s=13 TeV." Physics Letters B 772: 752-776.
    
Sirunyan, A. M., et al. (2017). "Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV." Physical Review D 96(11).
    
Sirunyan, A. M., et al. (2017). "Measurement of double-differential cross sections for top quark pair production in pp collisions at root s=8 TeV and impact on parton distribution functions." European Physical Journal C 77(7).
    
Sirunyan, A. M., et al. (2017). "Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(8).
    
Sirunyan, A. M., et al. (2017). "Measurement of the jet mass in highly boosted t(t)over-bar events from pp collisions at root s=8TeV." European Physical Journal C 77(7).
    
Sirunyan, A. M., et al. (2017). "Measurement of the semileptonic t(t)over-bar plus gamma production cross section in pp collisions at root s=8 TeV." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Measurement of the t(t)over-bar production cross section using events with one lepton and at least one jet in pp collisions at root s=13 TeV." Journal of High Energy Physics(9).
    
Sirunyan, A. M., et al. (2017). "Measurement of the top quark mass using single top quark events in proton-proton collisions at root s=8 TeV." European Physical Journal C 77(5).
    
Sirunyan, A. M., et al. (2017). "Measurement of the triple-differential dijet cross section in proton-proton collisions at root s=8 TeV and constraints on parton distribution functions." European Physical Journal C 77(11).
    
Sirunyan, A. M., et al. (2017). "Measurements of jet charge with dijet events in pp collisions at root s=8 TeV." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Measurements of the charm jet cross section and nuclear modification factor in pPb collisions at root sNN=5.02TeV." Physics Letters B 772: 306-329.
    
Sirunyan, A. M., et al. (2017). "Measurements of the pp -> W gamma gamma and pp -> Z gamma gamma cross sections and limits on anomalous quartic gauge couplings at root s=8 TeV." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Relative Modification of Prompt psi(2S) and J/psi Yields from pp to PbPb Collisions at root(S)(NN)=5.02 TeV." Physical Review Letters 118(16).
    
Sirunyan, A. M., et al. (2017). "Search for a heavy resonance decaying to a top quark and a vector-like top quark at root s=13 TeV." Journal of High Energy Physics(9).
    
Sirunyan, A. M., et al. (2017). "Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at root s=8 TeV." Journal of High Energy Physics(7).
    
Sirunyan, A. M., et al. (2017). "Search for associated production of dark matter with a Higgs boson decaying to b(b)over-bar or gamma gamma at root s=13 TeV." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Search for black holes and other new phenomena in high-multiplicity final states in proton-proton collisions at root s=13 TeV." Physics Letters B 774: 279-307.
    
Sirunyan, A. M., et al. (2017). "Search for Charged Higgs Bosons Produced via Vector Boson Fusion and Decaying into a Pair of W and Z Bosons Using pp Collisions at root s=13 TeV." Physical Review Letters 119(14).
    
Sirunyan, A. M., et al. (2017). "Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at root s = 13 TeV (vol 3, 061, 2017)." Journal of High Energy Physics(9).
    
Sirunyan, A. M., et al. (2017). "Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at root s=13 TeV." European Physical Journal C 77(12).
    
Sirunyan, A. M., et al. (2017). "Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at root S=13 TeV." Journal of High Energy Physics(7).
    
Sirunyan, A. M., et al. (2017). "Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states." Journal of High Energy Physics(4).
    
Sirunyan, A. M., et al. (2017). "Search for Higgs boson pair production in the bb tau state in proton-proton collisions at root(s)=8 TeV." Physical Review D 96(7).
    
Sirunyan, A. M., et al. (2017). "Search for high-mass Z gamma resonances in proton-proton collisions at root s=8 and 13 TeV using jet substructure techniques." Physics Letters B 772: 363-387.
    
Sirunyan, A. M., et al. (2017). "Search for massive resonances decaying in to WW,WZ or ZZ bosons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
    
Sirunyan, A. M., et al. (2017). "Search for new physics in the monophoton final state in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(10).
    
Sirunyan, A. M., et al. (2017). "Search for new physics with dijet angular distributions in proton-proton collisions at root S = 13 TeV." Journal of High Energy Physics(7).
    
Sirunyan, A. M., et al. (2017). "Search for single productio no vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(5).
    
Sirunyan, A. M., et al. (2017). "Search for single production of vector-like quarks decaying into a b quark and a W boson in proton-proton collisions at root s=13 TeV." Physics Letters B 772: 634-656.
    
Sirunyan, A. M., et al. (2017). "Search for t(t)over-bar resonances in highly boosted lepton plus jets and fully hadronic final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(7).
    
Sirunyan, A. M., et al. (2017). "Search for third-generation scalar leptoquarks and heavy right-handed neutrinos in final states with two tau leptons and two jets in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(7).
    
Sirunyan, A. M., et al. (2017). "Search for top quark partners with charge 5/3 in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(8).
    
Sirunyan, A. M., et al. (2017). "Searches for pair production of third-generation squarks in root s=13 TeV pp collisions." European Physical Journal C 77(5).
    
Sirunyan, A. M., et al. (2017). "Study of Jet Quenching with Z plus jet Correlations in Pb-Pb and pp Collisions at root s(NN)=5.02 TeV." Physical Review Letters 119(8).
    
Sirunyan, A. M., et al. (2017). "Particle-flow reconstruction and global event description with the CMS detector." Journal of Instrumentation 12.
    
Sirunyan, A. M., et al. (2017). "Mechanical stability of the CMS strip tracker measured with a laser alignment system." Journal of Instrumentation 12.
    
Sirunyan, A. M., et al. (2017). "Measurement of the B-+/- Meson Nuclear Modification Factor in Pb-Pb Collisions at root s(NN)=5.02 TeV." Physical Review Letters 119(15).
    
Sirunyan, A. M., et al. (2017). "Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
    
Sirunyan, A. M., et al. (2017). "Search for dijet resonances in proton-proton collisions at root s=13 TeV and constraints on dark matter and other models." Physics Letters B 769: 520-542.
    
Sirunyan, A. M., et al. (2017). "Search for new phenomena with the M-T2 variable in the all-hadronic final state produced in proton-proton collisions at root s=13TeV." European Physical Journal C 77(10).
    
Sirunyan, A. M., et al. (2017). "Observation of Top Quark Production in Proton-Nucleus Collisions." Physical Review Letters 119(24).
    
Turan, H. T., Yavuz, I., et al. (2017). "Understanding the Impact of Thiophene/Furan Substitution on Intrinsic Charge-Carrier Mobility." Journal of Physical Chemistry C 121(46): 25682-25690.
    
Yavuz, I. (2017). "Below-threshold harmonic generation from strong non-uniform fields." Journal of Modern Optics 64(19): 2043-2050.
    
Yavuz, I. and K. N. Houk (2017). "Mesoscale Ordering and Charge-Transport of Crystalline Spiro-OMeTAD Organic Semiconductors." Journal of Physical Chemistry C 121(2): 993-999.
    
Yavuz, I. and S. A. Lopez (2017). "Understanding dispersive charge-transport in crystalline organic-semiconductors." Physical Chemistry Chemical Physics 19(1): 231-236.
    
Zerenturk, A., et al. (2017). "Low temperature EPR investigation of Co2+ ion doped into rutile TiO2 single crystal: Experiments and simulations." Journal of magnetism and magnetic materials 423: 145-151.
    
Zerenturk, A., et al. (2017). "Experimental and theoretical investigations on low temperature EPR of Cu2+ centers in TiO2 rutile single crystal." Journal of Alloys and Compounds 710: 836-842.
    


2016

 

 

1. Akyurek, T., L. P. Tucker, X. Liu, and S. Usman. "Portable Spectroscopic Fast Neutron Probe and He-3 Detector Dead-Time Measurements." Progress in Nuclear Energy 92,  (2016): 15-21.

2. Alevli, M., N. Gungor, A. Haider, S. Kizir, S. A. Leghari, and N. Biyikli. "Substrate Temperature Influence on the Properties of Gan Thin Films Grown by Hollow-Cathode Plasma-Assisted Atomic Layer Deposition." Journal of Vacuum Science & Technology A 34, no. 1 (2016).

3. Alevli, M., A. Haider, S. Kizir, S. A. Leghari, and N. Biyikli. "Comparison of Trimethylgallium and Triethylgallium as "Ga" Source Materials for the Growth of Ultrathin Gan Films on Si (100) Substrates Via Hollow-Cathode Plasma-Assisted Atomic Layer Deposition." Journal of Vacuum Science & Technology A 34, no. 1 (2016).

4. Arifa, H., A. Boukhachem, B. Askri, K. Boubaker, A. Yumak, and K. Raouadi. "Structural, Optical and Conductivity Investigations on Kappa-Al2o3 Ceramics for Powder Metallurgical Production and Sensitivity Applications." Ceramics International 42, no. 2 (2016): 2147-2157.

5. Basak, A. S., M. K. Ekmekci, M. Erdem, M. Ilhan, and A. Mergen. "Investigation of Boron-Doping Effect on Photoluminescence Properties of Cdnb2o6: Eu3+ Phosphors." Journal of Fluorescence 26, no. 2 (2016): 719-724.

6. Boukhachem, A., A. Ziouche, M. Ben Amor, O. Kamoun, M. Zergoug, H. Maghraoui-Meherzi, A. Yumak, K. Boubaker, and M. Amlouk. "Physical Investigations on Perovskite Lamno3-Delta Sprayed Thin Films for Spintronic Applications." Materials Research Bulletin 74,  (2016): 202-211.

7. Chowdhury, F. I., A. Alnuaimi, S. Alkis, B. Ortac, S. Akturk, M. Alevli, N. Dietz, A. K. Okyay, and A. Nayfeh. "Enhancement in C-Si Solar Cells Using 16 Nm Inn Nanoparticles." Materials Research Express 3, no. 5 (2016).

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9. Deger, C., M. Ozdemir, and F. Yildiz. "Magnetostatic Spin Wave Resonance in Square-Patterned Ni0.77fe0.16cu0.05cr0.02 (Mu-Metal) Thinfilms." Journal of Magnetism and Magnetic Materials 408,  (2016): 13-17.

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12. Ekmekci, M. K., M. Erdem, A. S. Basak, and O. Danis. "Structural and Optical Properties of Nd3+ Doped Columbite Srnb2o6." Optik 127, no. 8 (2016): 4123-4126.

13. Ekmekci, M. K., M. Erdem, M. Ilhan, A. S. Basak, and A. Mergen. "Synthesis, Characterization and Photoluminescence Properties of Eu3+ Doped Columbite Cdnb2o6." Optik 127, no. 4 (2016): 1918-1921.

14. Erdem, M., G. Eryurek, A. Mergen, and B. Di Bartolo. "Pressure Effects on the Cooperative Emission of Yb3+ : Y2si2o7 Nano-Powders." Ceramics International 42, no. 1 (2016): 1501-1506.

15. Kamoun, O., A. Boukhachem, C. Mrabet, A. Yumak, P. Petkova, K. Boubaker, and M. Amlouk. "Effect of Europium Content on Physical Properties of In2o3 Thin Films for Sensitivity and Optoelectronic Applications." Bulletin of Materials Science 39, no. 3 (2016): 777-788.

16. Kamoun, O., A. Boukhachem, A. Yumak, P. Petkova, K. Boubaker, and M. Amlouk. "Europium Incorporation Dynamics and Some Physical Investigations within Zno Sprayed Thin Films." Materials Science in Semiconductor Processing 43,  (2016): 8-16.

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19. Petkova, P., K. Boubaker, P. Vasilev, M. Mustafa, A. Yumak, and D. Bachvarova. "Common and Different Doping Patterns within Photo-Reactive Complexes of Co2+ in Bi12sio20 and Co3+ in Bi12tio20." Optik 127, no. 9 (2016): 3925-3928.

20. Petkova, P., K. Boubaker, P. Vasilev, M. Mustafa, A. Yumak, H. Touihri, and M. T. Soltani. "Infrared Spectroscopy of Undoped and Cu-Doped (80-X)Sb2o3-20li(2)O-Xmoo(3) Glasses." In Proceedings of the 5th International Congress in Advances in Applied Physics and Materials Science Congress & Exhibition, edited by A. Y. Oral, Z. B. B. Oral, M. E. Akoz, M. Sezer and S. Kol, 1727, 2016.

21. Pienkos, J. A., A. D. Agakidou, C. O. Trindle, D. W. Herwald, Z. Altun, and P. S. Wagenknecht. "Titanocene as a New Acceptor (a) for Arylamine Donors (D) in D-Pi-a Chromophores." Organometallics 35, no. 16 (2016): 2575-2578.

22. Saafi, I., R. Dridi, R. Mimouni, A. Amlouk, A. Yumak, K. Boubaker, P. Petkova, and M. Amlouk. "Microstructural and Optical Properties of Sno2-Znsno3 Ceramics." Ceramics International 42, no. 5 (2016): 6273-6281.

23. Sahin, S., E. A. Bleda, Z. Altun, and C. Trindle. "Computational Characterization of Isomeric C4h2o Systems: Thermochemistry, Vibrational Frequencies, and Optical Spectra for Butatrienone, Ethynyl Ketene, Butadiynol, and Triafulvenone." International Journal of Quantum Chemistry 116, no. 6 (2016): 444-451.

24. Tikman, Y., I. Yavuz, M. F. Ciappina, A. Chacon, Z. Altun, and M. Lewenstein. "High-Order-Harmonic Generation from Rydberg Atoms Driven by Plasmon-Enhanced Laser Fields." Physical Review A 93, no. 2 (2016).

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26. Unal, H., U. A. Kaya, K. Esmer, A. Mimaroglu, and B. Poyraz. "Influence of Wax Content on the Electrical, Thermal and Tribological Behaviour of a Polyamide 6/Graphite Composite." Journal of Polymer Engineering 36, no. 3 (2016): 279-286.

27. Yavuz, I., M. F. Ciappina, A. Chacon, Z. Altun, M. F. Kling, and M. Lewenstein. "Controlling Electron Localization in H-2(+) by Intense Plasmon-Enhanced Laser Fields." Physical Review A 93, no. 3 (2016).

28. Yumak, A., S. Goumri-Said, W. Khan, K. Boubaker, and P. Petkova. "Doping-Induced Stability in Vanadium-Doped Zno Quantum Well Wires (Qww): Combination of Dft Calculations within Experimental Measurements." Solid State Sciences 57,  (2016): 33-37.

29. Yumak, A., U. Yahsi, P. Petkova, and K. Boubaker. "Europium Doping-Induced Stability and Quantum Confinement Effect in Zno Quantum Well Wires Qww: Electronic Structure Calculation and Material Structural Investigation in Terms of Band-Gap Shift." Materials Letters 164,  (2016): 89-92.

30) Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV.By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1611.06594 [hep-ex]].10.3204/PUBDB-2016-05677.JHEP (2016).

31) Observation of $\Upsilon(\mathrm{1S})$ pair production in proton-proton collisions at $\sqrt{s} = $ 8 TeV.By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1610.07095 [hep-ex]].10.3204/PUBDB-2016-04888.JHEP (2016).

32) Search for long-lived charged particles in proton-proton collisions at sqrt(s) = 13 TeV.By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1609.08382 [hep-ex]].10.1103/PhysRevD.94.112004.Phys.Rev. D94 (2016) 112004.

33) Studies of inclusive four-jet production with two b-tagged jets in proton-proton collisions at 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1609.03489 [hep-ex]].10.1103/PhysRevD.94.112005.Phys.Rev. D94 (2016) 112005.

34) Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1609.02466 [nucl-ex]].10.1007/JHEP11(2016)055.JHEP 1611 (2016) 055.

35) Measurement of the ZZ production cross section and Z $\to \ell^+\ell^-\ell'^+\ell'^-$ branching fraction in pp collisions at $\sqrt s$=13 TeV.By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1607.08834 [hep-ex]].10.1016/j.physletb.2016.10.054.Phys.Lett. B763 (2016) 280-303.

36) Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV.By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1607.06975 [hep-ex]].10.1007/JHEP11(2016)147.JHEP 1611 (2016) 147.

37) Search for lepton flavour violating decays of the Higgs boson to $e τ\tau$ and $e \mu$ in proton–proton collisions at $\sqrt s=$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1607.03561 [hep-ex]].10.1016/j.physletb.2016.09.062, 10.3204/PUBDB-2016-04744.Phys.Lett. B763 (2016) 472-500.

38) Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $\sqrt{s}$ = 13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1607.00915 [hep-ex]].10.1007/JHEP12(2016)013.JHEP 1612 (2016) 013.

39) Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1607.00837 [hep-ex]].10.1103/PhysRevD.94.052006.Phys.Rev. D94 (2016) no.5, 052006.

40) Search for Resonant Production of High-Mass Photon Pairs in Proton-Proton Collisions at $\sqrt s$ =8 and 13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1606.04093 [hep-ex]].10.1103/PhysRevLett.117.051802.Phys.Rev.Lett. 117 (2016) no.5, 051802.

41) Phenomenological MSSM interpretation of CMS searches in pp collisions at sqrt(s) = 7 and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1606.03577 [hep-ex]].10.1007/JHEP10(2016)129.JHEP 1610 (2016) 129.

42) Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at $ \sqrt{s}=7 $ and 8 TeV. By ATLAS and CMS Collaborations (Georges Aad , ..., Mithat Kaya et al.).[arXiv:1606.02266 [hep-ex]].10.1007/JHEP08(2016)045.JHEP 1608 (2016) 045.

43) Measurement of the W boson helicity fractions in the decays of top quark pairs to lepton $+$ jets final states produced in pp collisions at $\sqrt s=$ 8TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1605.09047 [hep-ex]].10.1016/j.physletb.2016.10.007.Phys.Lett. B762 (2016) 512-534.

44) Search for supersymmetry in pp collisions at $ \sqrt{s}=13 $ TeV in the single-lepton final state using the sum of masses of large-radius jets. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1605.04608 [hep-ex]].10.1007/JHEP08(2016)122.JHEP 1608 (2016) 122.

45) Measurement of the double-differential inclusive jet cross section in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1605.04436 [hep-ex]].10.1140/epjc/s10052-016-4286-3.Eur.Phys.J. C76 (2016) no.8, 451.

46) Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1605.03171 [hep-ex]].10.1140/epjc/s10052-016-4261-z.Eur.Phys.J. C76 (2016) no.8, 439.

47) Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1605.02329 [hep-ex]].10.1007/JHEP09(2016)051.JHEP 1609 (2016) 051.

48) Measurement of the integrated and differential $t \bar t$ production cross sections for high-$p_t$ top quarks in $pp$ collisions at $\sqrt s =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1605.00116 [hep-ex]].10.1103/PhysRevD.94.072002.Phys.Rev. D94 (2016) no.7, 072002.

49) Search for narrow resonances in dijet final states at $\sqrt(s)=$ 8 TeV with the novel CMS technique of data scouting. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1604.08907 [hep-ex]].10.1103/PhysRevLett.117.031802.Phys.Rev.Lett. 117 (2016) no.3, 031802.

50) Search for lepton flavour violating decays of heavy resonances and quantum black holes to an e$\mu$ pair in proton-proton collisions at $\sqrt{s}$ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1604.05239 [hep-ex]].10.1140/epjc/s10052-016-4149-y.Eur.Phys.J. C76 (2016) no.6, 317.

51) Evidence for exclusive $\gamma\gamma \to W^+ W^-$ production and constraints on anomalous quartic gauge couplings in $pp$ collisions at $ \sqrt{s}=7 $ and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1604.04464 [hep-ex]].10.1007/JHEP08(2016)119.JHEP 1608 (2016) 119.

52) Search for two Higgs bosons in final states containing two photons and two bottom quarks in proton-proton collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.06896 [hep-ex]].10.1103/PhysRevD.94.052012.Phys.Rev. D94 (2016) no.5, 052012.

53) Measurement of the top quark mass using charged particles in pp collisions at $\sqrt s =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.06536 [hep-ex]].10.1103/PhysRevD.93.092006.Phys.Rev. D93 (2016) no.9, 092006.

54) Measurements of $t \bar t$ charge asymmetry using dilepton final states in pp collisions at $\sqrt s=8$ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.06221 [hep-ex]].10.1016/j.physletb.2016.07.006.Phys.Lett. B760 (2016) 365-386.

55) Search for new physics with the M$_{T2}$ variable in all-jets final states produced in pp collisions at $ \sqrt{s}=13 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.04053 [hep-ex]].10.1007/JHEP10(2016)006.JHEP 1610 (2016) 006.

56) Search for neutral resonances decaying into a Z boson and a pair of b jets or tau leptons. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.02991 [hep-ex]].10.1016/j.physletb.2016.05.087.Phys.Lett. B759 (2016) 369-394.

57) $\Upsilon(\mathrm{nS})$ polarizations versus particle multiplicity in pp collisions at $\sqrt{s} =$ 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.02913 [hep-ex]].10.1016/j.physletb.2016.07.065.Phys.Lett. B761 (2016) 31-52.

58) Search for s channel single top quark production in pp collisions at $ \sqrt{s}=7 $ and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.02555 [hep-ex]].10.1007/JHEP09(2016)027.JHEP 1609 (2016) 027.

59) Measurement of the t-tbar production cross section in the e-mu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.02303 [hep-ex]].10.1007/JHEP08(2016)029.JHEP 1608 (2016) 029.

60) Search for heavy Majorana neutrinos in e$^{±}$e$^{±}$+ jets and e$^{±}$ $\mu^{±}$+ jets events in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.02248 [hep-ex]].10.1007/JHEP04(2016)169.JHEP 1604 (2016) 169.

61) Measurement of the differential cross section and charge asymmetry for inclusive $\mathrm {p}\mathrm {p}\rightarrow \mathrm {W}^{\pm }+X$ production at ${\sqrt{s}} = 8$ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.01803 [hep-ex]].10.1140/epjc/s10052-016-4293-4.Eur.Phys.J. C76 (2016) no.8, 469.

62) Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s} = 8\;\text {TeV} $. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1603.00765 [hep-ex]].10.1140/epjc/s10052-016-4292-5.Eur.Phys.J. C76 (2016) no.8, 460.

63) Search for supersymmetry in electroweak production with photons and large missing transverse energy in pp collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.08772 [hep-ex]].10.1016/j.physletb.2016.05.088.Phys.Lett. B759 (2016) 479-500.

64) Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.08762 [hep-ex]].10.1140/epjc/s10052-016-4206-6.Eur.Phys.J. C76 (2016) no.7, 371.

65) Measurement of the $ \mathrm{ Z } \gamma \rightarrow \nu \bar{\nu} \gamma$ production cross section in pp collisions at $\sqrt{s}=$ 8 TeV and limits on anomalous $ \mathrm{ ZZ } \gamma$ and $ \mathrm{Z} \gamma \gamma$ trilinear gauge boson couplings. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.07152 [hep-ex]].10.1016/j.physletb.2016.06.080.Phys.Lett. B760 (2016) 448-468.

66) Search for supersymmetry in the multijet and missing transverse momentum final state in pp collisions at 13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.06581 [hep-ex]].10.1016/j.physletb.2016.05.002.Phys.Lett. B758 (2016) 152-180.

67) Measurement of dijet azimuthal decorrelation in pp collisions at $\sqrt{s}=8\,\mathrm{TeV} $. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.04384 [hep-ex]].10.1140/epjc/s10052-016-4346-8.Eur.Phys.J. C76 (2016) no.10, 536.

68) Search for R-parity violating decays of a top squark in proton-proton collisions at $\sqrt{s}$ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.04334 [hep-ex]].10.1016/j.physletb.2016.06.039.Phys.Lett. B760 (2016) 178-201.

69) Combined search for anomalous pseudoscalar HVV couplings in VH(H $\to b \bar b$) production and H $\to$ VV decay. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.04305 [hep-ex]].10.1016/j.physletb.2016.06.004.Phys.Lett. B759 (2016) 672-696.

70) Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).arXiv:1602.03169 [hep-ex]].10.1007/JHEP09(2016)056, 10.1007/JHEP07(2016)027.JHEP 1607 (2016) 027, Erratum: JHEP 1609 (2016) 056.

71) Search for supersymmetry in pp collisions at sqrt(s) = 8 TeV in final states with boosted W bosons and b jets using razor variables. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1602.02917 [hep-ex]].10.1103/PhysRevD.93.092009.Phys.Rev. D93 (2016) no.9, 092009.

72) Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at $ \sqrt{s}=7 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1601.06713 [hep-ex]].10.1007/JHEP08(2016)139.JHEP 1608 (2016) 139.

73) Search for massive WH resonances decaying into the $\ell \nu \mathrm{b} \overline{\mathrm{b}} $ final state at $\sqrt{s}=8$ $~\text {TeV}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1601.06431 [hep-ex]].10.1140/epjc/s10052-016-4067-z.Eur.Phys.J. C76 (2016) no.5, 237.

74) Forward–backward asymmetry of Drell–Yan lepton pairs in pp collisions at sqrt (s) = 8 TeVBy CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1601.04768 [hep-ex]].10.1140/epjc/s10052-016-4156-z.Eur.Phys.J. C76 (2016) no.6, 325.

75) Measurement of inclusive jet production and nuclear modifications in pPb collisions at $\sqrt{s_{_\mathrm {NN}}} =$ 5.02 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1601.02001 [nucl-ex]].10.1140/epjc/s10052-016-4205-7.Eur.Phys.J. C76 (2016) no.7, 372.

76) Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV. By CMS Collaboration (V. Khachatryan, ..., M. Kaya et al.)[arXiv:1601.01107 [hep-ex]].10.1103/PhysRevD.93.052007.Phys.Rev. D93 (2016) no.5, 052007.

77) Correlations between jets and charged particles in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1601.00079 [nucl-ex]].10.1007/JHEP02(2016)156.JHEP 1602 (2016) 156.

78) Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at $ \sqrt{s}=7 $ and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1512.08377 [hep-ex]].10.1007/JHEP04(2016)005.JHEP 1604 (2016) 005.

79) Search for supersymmetry in events with soft leptons, low jet multiplicity, and missing transverse energy in proton–proton collisions at $\sqrt{s}$=8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1512.08002 [hep-ex]].10.1016/j.physletb.2016.05.033.Phys.Lett. B759 (2016) 9-35.

80) Study of Z boson production in pPb collisions at $\sqrt {s NN }$=5.02TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1512.06461 [hep-ex]].10.1016/j.physletb.2016.05.044.Phys.Lett. B759 (2016) 36-57.

81) Measurement of the inclusive jet cross section in pp collisions at $\sqrt{s} = 2.76\,\text {TeV}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1512.06212 [hep-ex]].10.1140/epjc/s10052-016-4083-z.Eur.Phys.J. C76 (2016) no.5, 265.

82) Search for narrow resonances decaying to dijets in proton-proton collisions at $\sqrt(s) =$ 13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1512.01224 [hep-ex]].10.1103/PhysRevLett.116.071801.Phys.Rev.Lett. 116 (2016) no.7, 071801.

83) Event generator tunes obtained from underlying event and multiparton scattering measurements. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1512.00815 [hep-ex]].10.1140/epjc/s10052-016-3988-x.Eur.Phys.J. C76 (2016) no.3, 155.

84) Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at $\sqrt s=$ 8  TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1511.09375 [hep-ex]].10.1103/PhysRevD.93.052011.Phys.Rev. D93 (2016) no.5, 052011.

85) Measurement of spin correlations in $t\bar{t}$ production using the matrix element method in the muon+jets final state in pp collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1511.06170 [hep-ex]].10.1016/j.physletb.2016.05.005.Phys.Lett. B758 (2016) 321-346.

86) Search for anomalous single top quark production in association with a photon in pp collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1511.03951 [hep-ex]].10.1007/JHEP04(2016)035.JHEP 1604 (2016) 035.

87) Search for a low-mass pseudoscalar Higgs boson produced in association with a $b\bar{b}$ pair in pp collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1511.03610 [hep-ex]].10.1016/j.physletb.2016.05.003.Phys.Lett. B758 (2016) 296-320.

88) Measurement of top quark polarisation in t-channel single top quark production. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1511.02138 [hep-ex]].10.1007/JHEP04(2016)073.JHEP 1604 (2016) 073.

89) Search for excited leptons in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1511.01407 [hep-ex]].10.1007/JHEP03(2016)125.JHEP 1603 (2016) 125.

90) Reconstruction and identification of τ lepton decays to hadrons and ν$_τ$ at CMS. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.07488 [physics.ins-det]].10.1088/1748-0221/11/01/P01019.JINST 11 (2016) no.01, P01019.

91) Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into $\tau$ leptons in pp collisions at $\sqrt{s}=8$ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.06534 [hep-ex]].10.1007/JHEP01(2016)079.JHEP 1601 (2016) 079.

92) Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.05302 [hep-ex]].10.1103/PhysRevLett.116.052002.Phys.Rev.Lett. 116 (2016) no.5, 052002.

93) Search for a light charged Higgs boson decaying to $ \mathrm{c}\overline{\mathrm{s}} $ in pp collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.04252 [hep-ex]].10.1007/JHEP12(2015)178.JHEP 1512 (2015) 178.

94) Transverse momentum spectra of inclusive b jets in pPb collisions at $\sqrt{s_{NN}} = $ 5.02 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.03373 [nucl-ex]].10.1016/j.physletb.2016.01.010.Phys.Lett. B754 (2016) 59.

95) Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.03072 [hep-ex]].10.1140/epjc/s10052-016-4105-x.Eur.Phys.J. C76 (2016) no.7, 379.

96) Measurement of long-range near-side two-particle angular correlations in pp collisions at $\sqrt s =$13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.03068 [nucl-ex]].10.1103/PhysRevLett.116.172302.Phys.Rev.Lett. 116 (2016) no.17, 172302.

97) Searches for a heavy scalar boson H decaying to a pair of 125 GeV Higgs bosons hh or for a heavy pseudoscalar boson A decaying to Zh, in the final states with $h \to \tau \tau$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.01181 [hep-ex]].10.1016/j.physletb.2016.01.056.Phys.Lett. B755 (2016) 217-244.

98) Observation of top quark pairs produced in association with a vector boson in pp collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.01131 [hep-ex]].10.1007/JHEP01(2016)096.JHEP 1601 (2016) 096.

99) Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.09029 [nucl-ex]].10.1007/JHEP01(2016)006.JHEP 1601 (2016) 006.

100) Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.08159 [hep-ex]].10.1007/JHEP06(2016)177.JHEP 1606 (2016) 177.

101) Search for the production of an excited bottom quark decaying to $tW$ in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.08141 [hep-ex]].10.1007/JHEP01(2016)166.JHEP 1601 (2016) 166.

102) Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.06076 [hep-ex]].10.1140/epjc/s10052-016-3956-5.Eur.Phys.J. C76 (2016) no.3, 128.

103) Search for $W' \to tb$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.06051 [hep-ex]].10.1007/JHEP02(2016)122.JHEP 1602 (2016) 122.

104) Search for vector-like charge 2/3 T quarks in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.04177 [hep-ex]].10.1103/PhysRevD.93.012003.Phys.Rev. D93 (2016) no.1, 012003.

105) Measurement of the top quark mass using proton-proton data at ${\sqrt{(s)}}$ = 7 and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.04044 [hep-ex]].10.1103/PhysRevD.93.072004.Phys.Rev. D93 (2016) no.7, 072004.

106) Measurement of the inelastic cross section in proton–lead collisions at $\sqrt {s_{NN}}=$ 5.02 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.03893 [hep-ex]].10.1016/j.physletb.2016.06.027.Phys.Lett. B759 (2016) 641-662.

107) Search for single production of scalar leptoquarks in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.03750 [hep-ex]].10.1103/PhysRevD.93.032005.Phys.Rev. D93 (2016) no.3, 032005.

108) Search for pair production of first and second generation leptoquarks in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1509.03744 [hep-ex]].10.1103/PhysRevD.93.032004.Phys.Rev. D93 (2016) no.3, 032004.

109) Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at $\sqrt{s}=8\,\text {TeV} $. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.07819 [hep-ex]].10.1140/epjc/s10052-015-3853-3.Eur.Phys.J. C76 (2016) no.1, 13.

110) Study of B Meson Production in p$+$Pb Collisions at $\sqrt(s_{NN}=$5.02  TeV Using Exclusive Hadronic Decays. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.06678 [nucl-ex]].10.1103/PhysRevLett.116.032301.Phys.Rev.Lett. 116 (2016) no.3, 032301.

111) Search for W' decaying to tau lepton and neutrino in proton-proton collisions at $\sqrt(s) =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.04308 [hep-ex]].10.1016/j.physletb.2016.02.002.Phys.Lett. B755 (2016) 196-216.

112) Measurement of the charge asymmetry in top quark pair production in pp collisions at $\sqrt(s) =$ 8 TeV using a template method. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.03862 [hep-ex]].10.1103/PhysRevD.93.034014.Phys.Rev. D93 (2016) no.3, 034014.

113) Search for neutral MSSM Higgs bosons decaying to $\mu^{+} \mu^{-}$ in pp collisions at $ \sqrt{s} =$ 7 and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.01437 [hep-ex]].10.1016/j.physletb.2015.11.042.Phys.Lett. B752 (2016) 221-246.

114) Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in pp collisions at $\sqrt s=$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.01218 [hep-ex]].10.1016/j.physletb.2016.03.039.Phys.Lett. B757 (2016) 6-31.

115) Angular analysis of the decay $B^0 \to K^{*0} \mu^+ \mu^-$ from pp collisions at $\sqrt s = 8$ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.08126 [hep-ex]].10.1016/j.physletb.2015.12.020.Phys.Lett. B753 (2016) 424-448.

116) Measurement of the CP-violating weak phase $\phi_s$ and the decay width difference $\Delta \Gamma_s$ using the B$_s^0 \to J/\psi\phi$(1020) decay channel in pp collisions at $\sqrt{s}=$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.07527 [hep-ex]].10.1016/j.physletb.2016.03.046.Phys.Lett. B757 (2016) 97-120.

117) Search for pair-produced vectorlike B quarks in proton-proton collisions at $\sqrt{s}$=8  TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.07129 [hep-ex]].10.1103/PhysRevD.93.112009.Phys.Rev. D93 (2016) no.11, 112009.

118) Measurement of the ${{\mathrm{W} }^{+} }\mathrm{W}^{-} $ cross section in pp collisions at $\sqrt{s} =$ 8 TeV and limits on anomalous gauge couplings. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.03268 [hep-ex]].10.1140/epjc/s10052-016-4219-1.Eur.Phys.J. C76 (2016) no.7, 401.

119) Inclusive and differential measurements of the $t\overline{t}$ charge asymmetry in pp collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.)[arXiv:1507.03119 [hep-ex]].10.1016/j.physletb.2016.03.060.Phys.Lett. B757 (2016) 154-179.

120) Search for a Higgs boson decaying into $\gamma^* \gamma \to \ell \ell \gamma$ with low dilepton mass in pp collisions at $\sqrt s = $ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.03031 [hep-ex]].10.1016/j.physletb.2015.12.039.Phys.Lett. B753 (2016) 341-362.

121) Search for exotic decays of a Higgs boson into undetectable particles and one or more photons. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.00359 [hep-ex]].10.1016/j.physletb.2015.12.017.Phys.Lett. B753 (2016) 363-388.

122) Search for resonant $t \bar t$ production in proton-proton collisions at $\sqrt s=$ 8  TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1506.03062 [hep-ex]].10.1103/PhysRevD.93.012001.Phys.Rev. D93 (2016) no.1, 012001.

123) Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1506.01443 [hep-ex]].10.1007/JHEP02(2016)145.JHEP 1602 (2016) 145.

124) A search for pair production of new light bosons decaying into muons. By CMS Collaboration (V. Khachatryan, ..., M. Kaya et al.).[arXiv:1506.00424 [hep ex]]10.1016/j.physletb.2015.10.067. Phys.Lett. B752 (2016) 146-168.

125) Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1501.06089 [hep-ex]].10.1016/j.physletb.2016.02.047.Phys.Lett. B756 (2016) 84-102.

126) Search for new phenomena in monophoton final states in proton-proton collisions at $\sqrt s =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.). [arXiv:1410.8812 [hep-ex]].10.1016/j.physletb.2016.01.057.Phys.Lett. B755 (2016) 102-124.

127) Yavuz, I., Lopez, S. A., Lin, J. B. and Houk, K. N. "Quantitative prediction of morphology and electron transport in crystal and disordered organic semiconductors." Journal of Materials Chemistry C, 4, 11238-11243 (2016).

128) Benjamin P. Cherniawski, Steven Lopez, Edmund K Burnett, Ilhan Yavuz, Lei Zhang, Sean R. Parkin, Kendall N Houk and Alejandro Briseno "The Effect of Hexyl Side Chains on Molecular Conformations, Crystal Packing, and Charge Transport of Oligothiophenes." Journal of Materials Chemistry C, DOI:10.1039/C67C04612F (2016).

 
2015

1. Akbulut S, Akbulut A, Özdemir M, Yildiz F. Effect of deposition technique of Ni on the perpendicular magnetic anisotropy in Co/Ni multilayers. Journal of Magnetism and Magnetic Materials. 2015;390:137-41.
2. Akbulut S, Akbulut A, Özdemir M, Yildiz F. Effect of GaAs (100) substrate surface reconstruction on magnetic properties of Ni thin films. Journal of Magnetism and Magnetic Materials. 2015;373:155-9.
3. Alevli M, Gungor N, Alkis S, Ozgit-Akgun C, Donmez I, Okyay AK, et al. Effect of reactor pressure on optical and electrical properties of InN films grown by high-pressure chemical vapor deposition. Physica Status Solidi (C) Current Topics in Solid State Physics. 2015;12(4-5):423-9.
4. Alkis S, Chowdhury FI, Alevli M, Dietz N, Yalizay B, Aktürk S, et al. Enhancement of polycrystalline silicon solar cells efficiency using indium nitride particles. Journal of Optics (United Kingdom). 2015;17(10).
6. Anand S, Eryürek M, Karadag Y, Serpengüzel A, Kiraz A, editors. Efficient optical fiber coupling to whispering gallery modes of optically manipulated emulsion microdroplets. Progress in Electromagnetics Research Symposium; 2015.
8. Bayansal F, Gülen Y, Şahin B, Kahraman S, Çetinkara HA. CuO nanostructures grown by the SILAR method: Influence of Pb-doping on the morphological, structural and optical properties. Journal of Alloys and Compounds. 2015;619:378-82.
9. Baykal A, Delice Ö. Generalized Sparling–Thirring form in the Brans–Dicke theory. European Physical Journal C. 2015;75(2).
10. Ben Said L, Larbi T, Yumak A, Boubaker K, Amlouk M. Pure and zirconium-doped manganese(II,III) oxide: Investigations on structural and conduction-related properties within the Lattice Compatibility Theory scope. Materials Science in Semiconductor Processing. 2015;40:224-9.
12. Bleda EA, Tikman Y, Altun Z. Electron-Impact Ionization of Se16+ and Se17+ Ions. Journal of Physics: Conference Series. 2015;635(9).
13. Bleda EA, Trindle C, Altun Z. Studies on spin state preferences in Fe(II) complexes. Computational and Theoretical Chemistry. 2015;1073:139-48.
14. Boukhachem A, Kamoun O, Mrabet C, Mannai C, Zouaghi N, Yumak A, et al. Structural, optical, vibrational and photoluminescence studies of Sn-doped MoO3 sprayed thin films. Materials Research Bulletin. 2015;72:252-63.
15. Boukhachem A, Yumak A, Krichen S, Madani A, Abderrabba M, Petkova P, et al. Electrosynthesis and study of some physical properties of conductive and solid-state gas sensing polydiphenylamine. Sensors and Actuators, A: Physical. 2015;227:11-20.
16. Boyraz C, Urfa Y. Effect of solution molarity on microstructural and optical properties of CdCr2S4 thin films. Materials Science in Semiconductor Processing. 2015;36:1-6.
17. Chowdhury FI, Islam K, Alkis S, Ortaç B, Alevli M, Dietz N, et al., editors. Enhanced light scattering with energy downshifting using 16 nm indium nitride nanoparticles for improved thin-film a-Si N-i-P solar cells. ECS Transactions; 2015.
18. Çiftci DK, Delice O. Brans-Dicke-Maxwell solutions for higher dimensional static cylindrical symmetric spacetime. Journal of Mathematical Physics. 2015;56(7).
19. Colantoni A, Longo L, Boubaker K, Monarca D, Cecchini M, Cividino S, Yumak A et al. Lattice compatibility theory LCT investigations on sulfur-oxygen substitution during Sb2S3-Sb2O3 crystals growth. Materials Research Express. 2015;2(3).
20. Delice O, Durʇut T. Superradiance instability of small rotating AdS black holes in arbitrary dimensions. Physical Review D - Particles, Fields, Gravitation and Cosmology. 2015;92(2).
21. Dridi R, Saafi I, Mhamdi A, Matri A, Yumak A, Haj Lakhdar M, et al. Structural, optical and AC conductivity studies on alloy ZnO-Zn2SnO4 (ZnO-ZTO) thin films. Journal of Alloys and Compounds. 2015;634:179-86.
22. Duru IP, Değer C, Kalayci T, Arucu M. A computational study on magnetic effects of Zn 1 -xCrxO type diluted magnetic semiconductor. Journal of Magnetism and Magnetic Materials. 2015;396:268-74.
23. Ekmekçi MK, Erdem M, Başak AS. Molten salt synthesis, visible and near-IR region spectral properties of europium or neodymium doped CoNb2O6 columbite niobate. Dalton Transactions. 2015;44(12):5379-85.
24. Ekmekçi MK, Erdem M, Başak AS, Ilhan M, Mergen A. Molten salt synthesis and optical properties of Eu3+, Dy3+or Nd3+ doped NiNb2O6 columbite-type phosphors. Ceramics International. 2015;41(8):9680-5.
25. Erdem M, Ekmekci MK, Orucu H, Bilir G. Structural and Spectroscopic Properties of δ-Y2Si2O7 Nanopowders Activated with Nd3+ Ions. International Journal of Applied Ceramic Technology. 2015;12(5):1016-9.
26. Erdem M, Erguzel O, Ekmekci MK, Orucu H, Cinkaya H, Genc S, et al. Bright white up-conversion emission from sol-gel derived Yb3+/Er3+/Tm3+: Y2SiO5 nanocrystalline powders. Ceramics International. 2015.
27. Erdem M, Eryurek G, Di Bartolo B. White light emission from sol-gel derived γ-Y2Si2O7 nanoparticles. Journal of Alloys and Compounds. 2015;639:483-7.
28. Erdem M, Eryurek G, Di Bartolo B. Change of spectral output with pressure and white light generation in nanoscale Yb3+:Y2Si2O7. Optical Materials. 2015;49:90-3.
29. Erdem M, Ghafouri S, Ekmekçi MK, Mergen A, Ozen G. Structural and spectroscopic properties of Er3+:CdNb2O6phosphors. Nano-Structures for Optics and Photonics: Optical Strategies for Enhancing Sensing, Imaging, Communication and Energy Conversion2015. p. 443-5.
30. Erdem M, Ghafouri S, Ekmekçi MK, Mergen A, Özen G. Structural and spectroscopic properties of Er3+: CdNb2O6 phosphors. NATO Science for Peace and Security Series B: Physics and Biophysics2015. p. 443-5.
31. Erdem M, Ozen G, Yahsi U, Di Bartolo B. Thermal and size effect on the R lines luminescence in YAG:Cr3+. Journal of Luminescence. 2015;158:464-8.
32. Erdem M, Sitt B. Up conversion based white light emission from sol-gel derived α-Y2Si2O7 nanoparticles activated with Yb3+, Er3+ ions. Optical Materials. 2015;46:260-4.
33. Eryürek M, Karadag Y, Anand S, Kilinç N, Kiraz A, editors. Hydrogen and humidity sensing based on WGMs of elastic polymer optical microresonators. Progress in Electromagnetics Research Symposium; 2015.
34. Eryürek M, Karadag Y, Taşaltin N, Kilinç N, Kiraz A. Optical sensor for hydrogen gas based on a palladium-coated polymer microresonator. Sensors and Actuators, B: Chemical. 2015;212:78-83.
35. Eryürek M, Karadag Y, Taşaltm N, Kilinç N, Kiraz A, editors. Hydrogen gas sensing using palladium-coated microdisk microresonators. Proceedings of SPIE - The International Society for Optical Engineering; 2015.
36. Gherouel D, Yumak A, Znaidi M, Bouzidi A, Boubaker K, Yacoubi N, et al. Low-cost spray-processed Ag1-xCuxInS2 nano-films: Structural and functional investigation within the Lattice Compatibility Theory framework. Materials Research Bulletin. 2015;68:80-6.
37. Gülen Y. Synthesis and Characterization of Iron-Doped Lead Sulfide Thin Films. Metallurgical and Materials Transactions A: Physical Metallurgy and Materials Science. 2015;46(10):4698-704.
38. Guler A, Sertkol M, Saribaev L, Ozdemir M, Oner Y, Ross JH. Superconductivity in Pt-and La-Doped BaFe2As2 Compounds Prepared by Solid-State Reaction. IEEE Transactions on Magnetics. 2015;51(11).
39. Kirezli P, Delice Ö. Stationary axially symmetric solutions in Brans-Dicke theory. Physical Review D - Particles, Fields, Gravitation and Cosmology. 2015;92(10).
40. Larbi T, Amara A, Ouni B, Inoubli A, Karyaoui M, Yumak A, et al. Physical investigations on NiMn2O4 sprayed magnetic spinel for sensitivity applications. Journal of Magnetism and Magnetic Materials. 2015;387:139-46.
41. Madakbaş S, F, Eminoʇlu EM, Şen F, Kahraman MV. Preparation and electrical properties of polypyrrole containing photocured thiol-ene based composites. Progress in Organic Coatings. 2015;80:33-8.
42. Mhamdi A, Labidi A, Souissi B, Kahlaoui M, Yumak A, Boubaker K, et al. Impedance spectroscopy and sensors under ethanol vapors application of sprayed vanadium-doped ZnO compounds. Journal of Alloys and Compounds. 2015;639:648-58.
43. Mimouni R, Kamoun O, Yumak A, Mhamdi A, Boubaker K, Petkova P, et al. Effect of Mn content on structural, optical, opto-thermal and electrical properties of ZnO:Mn sprayed thin films compounds. Journal of Alloys and Compounds. 2015;645:100-11.
44. Orazymbetov K, Bleda EA, Altun Z, Topcu T. High-order harmonic generation from confined Rydberg atoms. Journal of Physics: Conference Series. 2015;635(9).
45. Özdemir ZG, Çataltepe ÖA, Onbaşli Ü. Impedance and dielectric properties of mercury cuprate at nonsuperconducting state. International Journal of Modern Physics B. 2015;29(29).
46. Saafi I, Dridi R, Mimouni R, Amlouk A, Yumak A, Boubaker K, et al. Microstructural and optical properties of SnO2-ZnSnO3 ceramics. Ceramics International. 2015.
47. Sahin-Dinc F, Sorrentino A, Tav C, Yahsi U. The Effect of Hole Fraction on Viscosity in Atactic and Syndiotactic Polystyrenes. International Journal of Thermophysics. 2015;36(10-11):3239-54.
48. Yahsi U, Coskun B, Yumak A, Boubaker K, Tav C. Relaxation time of polypropylene glycol and polypropylene glycol dimethylether-like polymers in terms of fluid-phase temperature and pressure dependent hole fraction. European Polymer Journal. 2015;68:226-32.
49. Yalçin O, Ünlüer Ş, Kazan S, Özdemir M, Öner Y. Temperature evolution of magnetic properties for (Cu/Co)60/Fe multilayer. Journal of Magnetism and Magnetic Materials. 2015;373:144-50.
50. Yavuz I, Tikman Y, Altun Z. High-order-harmonic generation from H2+ molecular ions near plasmon-enhanced laser fields. Physical Review A - Atomic, Molecular, and Optical Physics. 2015;92(2).
51. Yavuz I, Tikman Y, Altun Z. Harmonic-emission from Rydberg states in the vicinity of metallic nanostructures. Journal of Physics: Conference Series. 2015;635(12).
52. Yumak A, Boubaker K, Petkova P. An attempt to give exact solitary and periodic wave polynomial solutions to the nonlinear Klein-Gordon-Schrödinger equations. Chaos, Solitons and Fractals. 2015;81:299-302.
53. Yumak A, Boubaker K, Petkova P, Yahsi U. Molecular structure stability of short-chain chlorinated paraffins (SCCPs): Evidence from lattice compatibility and Simha-Somcynsky theories. Journal of Molecular Structure. 2015;1098:255-60.
54. Yumak A, Turgut G, Kamoun O, Ozisik H, Deligoz E, Petkova P, et al. Stability and morphology-dependence of Sc3+ ions incorporation and substitution kinetics within ZnO host lattice. Materials Science in Semiconductor Processing. 2015;39:103-11.
55. Zhou C, Xie T, Zhou R, Trindle CO, Tikman Y, Zhang X, et al. Waterborne Polyurethanes with Tunable Fluorescence and Room-Temperature Phosphorescence. ACS Applied Materials and Interfaces. 2015;7(31):17209-16.

56. Search for a light charged Higgs boson decaying to pp collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1510.04252 [hep-ex]]. 10.1007/JHEP12(2015)178. JHEP 1512 (2015) 178.

57) Search for a charged Higgs boson in pp collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.07774 [hep-ex]].10.1007/JHEP11(2015)018.JHEP 1511 (2015) 018.

58) Search for supersymmetry in the vector-boson fusion topology in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1508.07628 [hep-ex]].10.1007/JHEP11(2015)189. JHEP 1511 (2015) 189.

59) Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at sqrt(s) = 2.76 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.07229 [hep-ex]].10.1007/JHEP09(2015)137. JHEP 1509 (2015) 137.

60) Limits on the Higgs boson lifetime and width from its decay to four charged leptons.  By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.). [arXiv:1507.06656 [hep-ex]].10.1103/PhysRevD.92.072010.Phys.Rev. D92 (2015) no.7, 072010.

61) Pseudorapidity distribution of charged hadrons in proton-proton collisions at $\sqrt{s}$ = 13 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.05915 [hep-ex]].10.1016/j.physletb.2015.10.004.Phys.Lett. B751 (2015) 143-163.

62) Search for supersymmetry with photons in pp collisions at $\sqrt{s}$=8  TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.02898 [hep-ex]].10.1103/PhysRevD.92.072006.Phys.Rev. D92 (2015) no.7, 072006.

63) Production of leading charged particles and leading charged-particle jets at small transverse momenta in pp collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1507.00233 [hep-ex]].10.1103/PhysRevD.92.112001.Phys.Rev. D92 (2015) no.11, 112001.

64) Search for neutral MSSM Higgs bosons decaying into a pair of bottom quarks. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1506.08329 [hep-ex]].10.1007/JHEP11(2015)071.JHEP 1511 (2015) 071.

65) Search for diphoton resonances in the mass range from 150 to 850 GeV in pp collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1506.02301 [hep-ex]].10.1016/j.physletb.2015.09.062.Phys.Lett. B750 (2015) 494-519.

66) Search for the standard model Higgs boson produced through vector boson fusion and decaying to $b \overline{b}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1506.01010 [hep-ex]].10.1103/PhysRevD.92.032008. Phys.Rev. D92 (2015) no.3, 032008.

67) Search for neutral color-octet weak-triplet scalar particles in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1505.08118 [hep-ex]].10.1007/JHEP09(2015)201.JHEP 1509 (2015) 201.

68) Measurement of the differential cross section for top quark pair production in pp collisions at $\sqrt{s} = 8\,\text {TeV} $. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1505.04480 [hep-ex]].10.1140/epjc/s10052-015-3709-x. Eur.Phys.J. C75 (2015) no.11, 542.

69) Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in $ℓ^+ℓ^−b\overline{b}$ final states. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1504.04710 [hep-ex]] 10.1016/j.physletb.2015.07.010. Phys.Lett. B748 (2015) 221-243.

70) Angular coefficients of Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^+ \mu^-$ as a function of transverse momentum and rapidity. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1504.03512 [hep-ex]].10.1016/j.physletb.2015.08.061.Phys.Lett. B750 (2015) 154-175.

71) Measurement of the Z boson differential cross section in transverse momentum and rapidity in proton–proton collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1504.03511 [hep-ex]].10.1016/j.physletb.2015.07.065.Phys.Lett. B749 (2015) 187-209.

72) Search for the production of dark matter in association with top-quark pairs in the single-lepton final state in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1504.03198 [hep-ex]].10.1007/JHEP06(2015)121.JHEP 1506 (2015) 121.

73) Search for a Higgs boson in the mass range from 145 to 1000 GeV decaying to a pair of W or Z bosons. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1504.00936 [hep-ex]].10.1007/JHEP10(2015)144.JHEP 1510 (2015) 144.

74) Search for Third-Generation Scalar Leptoquarks in the t$\tau$ Channel in Proton-Proton Collisions at $\sqrt{s}$ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.09049 [hep-ex]].10.1007/JHEP11(2016)056, 10.1007/JHEP07(2015)042. JHEP 1507 (2015) 042, Erratum: JHEP 1611 (2016) 056.

75) Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.08689 [hep-ex]].10.1103/PhysRevD.92.012003.Phys.Rev. D92 (2015) no.1, 012003.

76) Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.08037 [hep-ex]].10.1007/JHEP06(2015)116.JHEP 1506 (2015) 116.

77) Combined Measurement of the Higgs Boson Mass in $pp$ Collisions at $\sqrt{s}=7$ and 8 TeV with the ATLAS and CMS Experiments. By ATLAS and CMS Collaborations (Georges Aad , ..., Mithat Kaya et al.).[arXiv:1503.07589 [hep-ex]].10.1103/PhysRevLett.114.191803.Phys.Rev.Lett. 114 (2015) 191803.

78) Study of W boson production in pPb collisions at $\sqrt{s_{\mathrm{NN}}} =$ 5.02 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.05825 [nucl-ex]].10.1016/j.physletb.2015.09.057.Phys.Lett. B750 (2015) 565-586.

79) Measurements of the $\mathrm{Z}$ $\mathrm{Z}$ production cross sections in the $2\mathrm{l} 2\nu $ channel in proton–proton collisions at $\sqrt{s} = 7$ and $8~\mathrm{TeV} $ and combined constraints on triple gauge couplings. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.05467 [hep-ex]].10.1140/epjc/s10052-015-3706-0. Eur.Phys.J. C75 (2015) no.10, 511.

80) Search for resonant pair production of Higgs bosons decaying to two bottom quark–antiquark pairs in proton–proton collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.04114 [hep-ex]].10.1016/j.physletb.2015.08.047.Phys.Lett. B749 (2015) 560-582.

81) Search for vector-like T quarks decaying to top quarks and Higgs bosons in the all-hadronic channel using jet substructure. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.01952 [hep-ex]].10.1007/JHEP06(2015)080.JHEP 1506 (2015) 080.

82) Evidence for transverse momentum and pseudorapidity dependent event plane fluctuations in PbPb and pPb collisions. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1503.01692 [nucl-ex]].10.1103/PhysRevC.92.034911.Phys.Rev. C92 (2015) no.3, 034911.

83) Study of Final-State Radiation in Decays of Z Bosons Produced in $pp$ Collisions at 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.07940 [hep-ex]].10.1103/PhysRevD.91.092012.Phys.Rev. D91 (2015) no.9, 092012.

84) Search for Lepton-Flavour-Violating Decays of the Higgs Boson. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.07400 [hep-ex]].10.1016/j.physletb.2015.07.053.Phys.Lett. B749 (2015) 337-362.

85) Search for Physics Beyond the Standard Model in Events with Two Leptons, Jets, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.06031 [hep-ex]].10.1007/JHEP04(2015)124.JHEP 1504 (2015) 124.

86) Measurement of the Zγ Production Cross Section in pp Collisions at 8 TeV and Search for Anomalous Triple Gauge Boson Couplings. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al [arXiv:1502.05664 [hep-ex]].10.1007/JHEP04(2015)164.JHEP 1504 (2015) 164.

87) Nuclear Effects on the Transverse Momentum Spectra of Charged Particles in pPb Collisions at $\sqrt{s_{_\mathrm {NN}}} =5.02$ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.[arXiv:1502.05387 [nucl-ex]].10.1140/epjc/s10052-015-3435-4.Eur.Phys.J. C75 (2015) no.5, 237.

88) Evidence for Collective Multiparticle Correlations in p-Pb Collisions. 

By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.05382 [nucl-ex]].10.1103/PhysRevLett.115.012301.Phys.Rev.Lett. 115 (2015) no.1, 012301.

89) Search for Narrow High-Mass Resonances in Proton–Proton Collisions at $\sqrt{s}$ = 8 TeV Decaying to a Z and a Higgs Boson. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.04994 [hep-ex]].10.1016/j.physletb.2015.07.011.Phys.Lett. B748 (2015) 255-277.

90) Distributions of Topological Observables in Inclusive Three- and Four-Jet Events in pp Collisions at sqrt(s) = 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.04785 [hep-ex]].10.1140/epjc/s10052-015-3491-9.Eur.Phys.J. C75 (2015) no.7, 302.

91) Searches for Supersymmetry using the M$_{T2}$ Variable in Hadronic Events Produced in pp Collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.04358 [hep-ex]].10.1007/JHEP05(2015)078.JHEP 1505 (2015) 078.

92) Measurement of J/ψ and ψ(2S) Prompt Double-Differential Cross Sections in pp Collisions at $\sqrt{s}$=7  TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.04155 [hep-ex]].10.1103/PhysRevLett.114.191802.Phys.Rev.Lett. 114 (2015) no.19, 191802.

93) Performance of Photon Reconstruction and Identification with the CMS Detector in Proton-Proton Collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.02702 [physics.ins-det]].10.1088/1748-0221/10/08/P08010.JINST 10 (2015) no.08, P08010.

94) Performance of Electron Reconstruction and Selection with the CMS Detector in Proton-Proton Collisions at √s = 8  TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.02701 [physics.ins-det]].10.1088/1748-0221/10/06/P06005.JINST 10 (2015) no.06, P06005.

95) Constraints on the pMSSM, AMSB model and on other models from the search for long-lived charged particles in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.02522 [hep-ex]].10.1140/epjc/s10052-015-3533-3.Eur.Phys.J. C75 (2015) no.7, 325.

96) Search for a Standard Model Higgs Boson Produced in Association with a Top-Quark Pair and Decaying to Bottom Quarks Using a Matrix Element Method. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.02485 [hep-ex]].10.1140/epjc/s10052-015-3454-1.Eur.Phys.J. C75 (2015) no.6, 251.

97) Search for Supersymmetry Using Razor Variables in Events with $b$-Tagged Jets in $pp$ Collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1502.00300 [hep-ex]].10.1103/PhysRevD.91.052018.Phys.Rev. D91 (2015) 052018.

98) Measurements of the $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) differential cross sections in pp collisions at $\sqrt{s} =$ 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1501.07750 [hep-ex]].10.1016/j.physletb.2015.07.037.Phys.Lett. B749 (2015) 14-34.

99) Search for Decays of Stopped Long-Lived Particles Produced in Proton–Proton Collisions at $\sqrt{s}= 8\,\text {TeV} $. 

By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1501.05603 [hep-ex]].10.1140/epjc/s10052-015-3367-z.Eur.Phys.J. C75 (2015) no.4, 151.

100) Search for heavy Majorana neutrinos in $\mu^\pm \mu^\pm+$ jets events in proton-proton collisions at $\sqrt{s}$ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1501.05566 [hep-ex]].10.1016/j.physletb.2015.06.070.Phys.Lett. B748 (2015) 144-166.

101) Search for resonances and quantum black holes using dijet mass spectra in proton-proton collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1501.04198 [hep-ex]].10.1103/PhysRevD.91.052009.Phys.Rev. D91 (2015) no.5, 052009.

102) Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 $\,\text {TeV}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1412.8662 [hep-ex]].10.1140/epjc/s10052-015-3351-7.Eur.Phys.J. C75 (2015) no.5, 212.

103) Search for pair-produced resonances decaying to jet pairs in proton–proton collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1412.7706 [hep-ex]].10.1016/j.physletb.2015.04.045.Phys.Lett. B747 (2015) 98-119.

104) Search for physics beyond the standard model in dilepton mass spectra in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1412.6302 [hep-ex]].10.1007/JHEP04(2015)025.JHEP 1504 (2015) 025.

105) Searches for supersymmetry based on events with b jets and four W bosons in pp collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1412.4109 [hep-ex]].10.1016/j.physletb.2015.04.002.Phys.Lett. B745 (2015) 5-28.

106) Measurement of the inclusive 3-jet production differential cross section in proton–proton collisions at 7 TeV and determination of the strong coupling constant in the TeV range. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1412.1633 [hep-ex]].10.1140/epjc/s10052-015-3376-y.Eur.Phys.J. C75 (2015) no.5, 186.

107) Measurements of differential and double-differential Drell-Yan cross sections in proton-proton collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1412.1115 [hep-ex]].10.1140/epjc/s10052-015-3364-2.Eur.Phys.J. C75 (2015) no.4, 147.

108) Search for stealth supersymmetry in events with jets, either photons or leptons, and low missing transverse momentum in pp collisions at 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.7255 [hep-ex]].10.1016/j.physletb.2015.03.017.Phys.Lett. B743 (2015) 503-525.

109) Search for long-lived particles that decay into final states containing two electrons or two muons in proton-proton collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.6977 [hep-ex]].10.1103/PhysRevD.91.052012.Phys.Rev. D91 (2015) no.5, 052012.

110) Search for Long-Lived Neutral Particles Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\sqrt{s} =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.6530 [hep-ex]].10.1103/PhysRevD.91.012007.Phys.Rev. D91 (2015) no.1, 012007.

111) Search for disappearing tracks in proton-proton collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (V. Khachatryan, ..., M. Kaya et al.).[arXiv:1411.6006 [hep-ex]].10.1007/JHEP01(2015)096.JHEP 1501 (2015) 096.

112) Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t} jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.5621 [hep-ex]].10.1016/j.physletb.2015.04.060.Phys.Lett. B746 (2015) 132-153.

113) Observation of the rare $B^0_s\to\mu^+\mu^-$ decay from the combined analysis of CMS and LHCb data. By CMS and LHCb Collaborations (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.4413 [hep-ex]].10.1038/nature14474.Nature 522 (2015) 68-72.

114) Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.3441 [hep-ex]].10.1103/PhysRevD.92.012004.Phys.Rev. D92 (2015) no.1, 012004.

115) Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton–proton collisions at $\sqrt s =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.2646 [hep-ex]].10.1016/j.physletb.2015.04.042.Phys.Lett. B746 (2015) 79-99.

116) Performance of the CMS missing transverse momentum reconstruction in pp data at $\sqrt{s}$ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1411.0511 [physics.ins-det]].10.1088/1748-0221/10/02/P02006.JINST 10 (2015) no.02, P02006.

117) Constraints on parton distribution functions and extraction of the strong coupling constant from the inclusive jet cross section in pp collisions at $\sqrt{s} = 7$ $\,\text {TeV}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1410.6765 [hep-ex]].10.1140/epjc/s10052-015-3499-1.Eur.Phys.J. C75 (2015) no.6, 288.

118) Search for a standard model-like Higgs boson in the $μ^+μ^−$ and $e^+e^−$ decay channels at the LHC. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1410.6679 [hep-ex]].10.1016/j.physletb.2015.03.048.Phys.Lett. B744 (2015) 184-207.

119) Study of vector boson scattering and search for new physics in events with two same-sign leptons and two jets. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1410.6315 [hep-ex]].10.1103/PhysRevLett.114.051801.Phys.Rev.Lett. 114 (2015) no.5, 051801.

120) Measurement of the ratio of the production cross sections times branching fractions of $B_{c}^{\pm} \to J/\psi \pi^{\pm}$ and $B^{\pm} \to J/\psi K^{\pm}$ and $\mathcal{B}(B_{c}^{\pm} \to J/\psi\pi^{\pm}\pi^{\pm}\pi^{\mp})/\mathcal{B}(B_{c}^{\pm} \to J/\psi \pi^{\pm})$ in pp collisions at $\sqrt{s} =$ 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.)[arXiv:1410.5729 [hep-ex]].10.1007/JHEP01(2015)063.JHEP 1501 (2015) 063.

121) Study of Z production in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV in the dimuon and dielectron decay channels. By CMS Collaboration (Serguei Chatrchyan, ..., Mithat Kaya et al.).[arXiv:1410.4825 [nucl-ex]].10.1007/JHEP03(2015)022.JHEP 1503 (2015) 022.

122) Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at $\sqrt{s}=8\,\text {TeV}$. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1410.3153 [hep-ex]].10.1140/epjc/s10052-014-3232-5.Eur.Phys.J. C75 (2015) no.2, 66.

123) Measurement of the W boson helicity in events with a single reconstructed top quark in pp collisions at $ \sqrt{s}=8 $ TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1410.1154 [hep-ex]].10.1007/JHEP01(2015)053.JHEP 1501 (2015) 053.

124) Search for Monotop Signatures in Proton-Proton Collisions at $\sqrt s =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1410.1149 [hep-ex]].10.1103/PhysRevLett.114.101801.Phys.Rev.Lett. 114 (2015) no.10, 101801.

125) Measurement of the production cross section ratio $\sigma$(Xb2(1P)) / $\sigma$(Xb1(1P) in pp collisions at $\sqrt s $ = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1409.5761 [hep-ex]].10.1016/j.physletb.2015.02.048.Phys.Lett. B743 (2015) 383-402.

126) Search for Displaced Supersymmetry in events with an electron and a muon with large impact parameters. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1409.4789 [hep-ex]].10.1103/PhysRevLett.114.061801.Phys.Rev.Lett. 114 (2015) no.6, 061801.

127) Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1409.3392 [nucl-ex]].10.1016/j.physletb.2015.01.034.Phys.Lett. B742 (2015) 200-224.

128) Search for dark matter, extra dimensions, and unparticles in monojet events in proton–proton collisions at sqrt (s) = 8TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1408.3583 [hep-ex]].10.1140/epjc/s10052-015-3451-4.Eur.Phys.J. C75 (2015) no.5, 235.

129) Measurements of jet multiplicity and differential production cross sections of $Z +$ jets events in proton-proton collisions at $\sqrt{s} =$ 7 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1408.3104 [hep-ex]].10.1103/PhysRevD.91.052008.Phys.Rev. D91 (2015) no.5, 052008.

130) Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at sqrt(s) = 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1408.2745 [hep-ex]].10.1103/PhysRevD.91.092005.Phys.Rev. D91 (2015) no.9, 092005.

131) Search for new resonances decaying via WZ to leptons in proton-proton collisions at $\sqrt s =$ 8 TeV. By CMS Collaboration (Vardan Khachatryan, ..., Mithat Kaya et al.).[arXiv:1407.3476 [hep-ex]].10.1016/j.physletb.2014.11.026.Phys.Lett. B740 (2015) 83-104.


2014

1. Akyar L, Delice Ö. On generalized Einstein-Rosen waves in Brans-Dicke theory. European Physical Journal Plus. 2014;129(10).
2. Akyar L, Delice Ö. On generalized Einstein-Rosen waves in Brans-Dicke theory. Journal of Applied Genetics. 2014;129(10).
3. Altun Z, Bleda EA, Trindle C, Wang J. Thermochemistry of N-heterocyclic carbenes with 5-, 4-, 3-, and 2-membered rings. International Journal of Quantum Chemistry. 2014;114(10):675-87.
4. Çimen Y, Ermiş E, Dumludaǧ F, Özkaya AR, Salih B, Bekaroǧlu O. Synthesis, characterization, electrochemistry and VOC sensing properties of novel ball-type dinuclear metallophthalocyanines. Sensors and Actuators, B: Chemical. 2014;202:1137-47.
5. Coşkun M, Dumludağ F, Altindal A. Solution processing grown Alq3 microwires for volatile organic compound vapor sensing. Sensor Letters. 2014;12(11):1583-9.
6. Dinc FS, Sedlacek T, Tav C, Yahsi U. On the non-newtonian viscous behavior of polymer melts in terms of temperature and pressure-dependent hole fraction. Journal of Applied Polymer Science. 2014;131(15).
7. Ekmekçi MK, Erdem M, Mergen A, Özen G, Bartolo BD. Molten salt synthesis and spectral properties of Nd3+ doped CdNb2O6 columbite phosphors. Journal of Alloys and Compounds. 2014;591:230-3.
8. Erdem M, Ekmekci MK, Orucu H, Bilir G. Structural and Spectroscopic Properties of δ-Y2Si2O7 Nanopowders Activated with Nd3+ Ions. International Journal of Applied Ceramic Technology. 2014.
9. Ghafouri SA, Erdem M, Ekmekçi MK, Mergen A, Özen G. Concentration effect of Er3+ions on structural and spectroscopic properties of CdNb2O6phosphors. Materials Research Bulletin. 2014;60:562-5.
10. Gülen Y. Characteristics of Ba-doped PbS thin films prepared by the SILAR method. Acta Physica Polonica A. 2014;126(3):763-7.
11. Gülen Y, Sahin B, Bayansal F, Çetinkara HA. Solution-phase synthesis of un-doped and Pb doped CdO films. Superlattices and Microstructures. 2014;68:48-55.
12. Kalaycι T, Bardakçι B. A spectroscopic investigation for the adsorption of 4-nitrophenol onto synthetic zeolites. Protection of Metals and Physical Chemistry of Surfaces. 2014;50(6):709-14.
13. Kaya AU, Güner S, Esmer K. Effects of solution mixing temperature on dielectric properties of PMMA/Pristine bentonite nanocomposites. Journal of Applied Polymer Science. 2014;131(4).
14. Madakbaş S, Çelik Z, Dumludaǧ F, Kahraman MV. Preparation, characterization and electrical properties of polyacrylonitrile/huntite composites. Polymer Bulletin. 2014;71(6):1471-81.
15. Madakbaş S, Şen F, Kahraman MV, Dumludağ F. Preparation, characterization, thermal, and dielectric properties of polypyrrole/h-BN nanocomposites. Advances in Polymer Technology. 2014;33(4).
16. Sahin B, Gülen Y, Bayansal F, Çetinkara HA, Güder HS. Structural and optical properties of Ba-doped CdO films prepared by SILAR method. Superlattices and Microstructures. 2014;65:56-63.
17. Tekcan B, Alkis S, Alevli M, Dietz N, Ortac B, Biyikli N, et al. A near-infrared range photodetector based on indium nitride nanocrystals obtained through laser ablation. IEEE Electron Device Letters. 2014;35(9):936-8.
18. Topkaya R, Kazan S, Yilgin R, Akdoǧan N, Özdemir M, Aktaş B. Ferromagnetic resonance studies of exchange biased CoO/Fe bilayer grown on MgO substrate. Journal of Superconductivity and Novel Magnetism. 2014;27(6):1503-12.
19. Yavuz I, Bleda EA, Altun Z, Topcu T. Phase-dependent interference fringes in the wavelength scaling of harmonic efficiency. Physical Review A - Atomic, Molecular, and Optical Physics. 2014;89(5).
20. Yilmaz O, Kayahan E, Gören F, Dumludag F. Methanol vapor sensing by porous silicon. Acta Physica Polonica A. 2014;125(2):288-9.
21. Khachatryan V, ...Kaya M..., et al. Search for standard model production of four top quarks in the lepton plus jets channel in pp collisions at root S=8 TeV. Journal of High Energy Physics. 2014(11).
22. Khachatryan V, ...Kaya M..., et al. Searches for heavy Higgs bosons in two-Higgs-doublet models and for t -> ch decay using multilepton and diphoton final states in pp collisions at 8 TeV. Physical Review D. 2014;90(11).
23. Khachatryan V, ...Kaya M..., et al. Constraints on the Higgs boson width from off-shell production and decay to Z-boson pairs. Physics Letters B. 2014;736:64-85.
24. Khachatryan V, ...Kaya M..., et al. Search for the associated production of the Higgs boson with a top-quark pair. Journal of High Energy Physics. 2014(9).
25. Khachatryan V, ...Kaya M..., et al. Measurement of top quark-antiquark pair production in association with a W or Z boson in pp collisions at root s=8 TeV. European Physical Journal C. 2014;74(9).
26. Khachatryan V, ...Kaya M..., et al. Search for the associated production of the Higgs boson with a top-quark pair (vol 9, 087, 2014). Journal of High Energy Physics. 2014(10).
27. Khachatryan V, ...Kaya M..., et al. Search for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisions. Journal of High Energy Physics. 2014(10).
28. Khachatryan V, ...Kaya M..., et al. Searches for electroweak neutralino and chargino production in channels with Higgs, Z, and W bosons in pp collisions at 8 TeV. Physical Review D. 2014;90(9).
29. Khachatryan V, ...Kaya M..., et al. Identification techniques for highly boosted W bosons that decay into hadrons. Journal of High Energy Physics. 2014(12).
30. Khachatryan V, ...Kaya M..., et al. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at v root s=8 TeV. Physics Letters B. 2014;739:229-49.
31. Khachatryan V, ...Kaya M..., et al. Measurement of the t(t)over-bar production cross section in pp collisions at root s=8 TeV in dilepton final states containing one tau lepton. Physics Letters B. 2014;739:23-43. 2013  1. Acharya AR, Gamage


2013

1. S, Senevirathna MKI, Alevli M, Bahadir K, Melton AG, et al. Thermal stability of InN epilayers grown by high pressure chemical vapor deposition. Applied Surface Science. 2013;268:1-5.
2. Akkoyunlu BO, Dogruel M, Tayanc M, Oruc I. Design and construction of a computer controlled automatic sequential rain sampler. Biotechnology and Biotechnological Equipment. 2013;27(3):3890-5.
3. Ali S, Mahmood S, Orban I, Altun Z, Schuch R, editors. Experimental recombination rate coefficients of B-like carbon and B-like neon. Physica Scripta; 2013.
4. Baykal A, Delice O. Multi-scalar-tensor equivalents for modified gravitational actions. Physical Review D - Particles, Fields, Gravitation and Cosmology. 2013;88(8).
5. Bayrak R, Dumludaǧ F, Akçay HT, Deǧirmencioǧlu I. Synthesis, characterization and electrical properties of peripherally tetra-aldazine substituted novel metal free phthalocyanine and its zinc(II) and nickel(II) complexes. Spectrochimica Acta - Part A: Molecular and Biomolecular Spectroscopy. 2013;105:550-6.
6. Bayrakdar H, Yalçin O, Vural S, Esmer K. Effect of different doping on the structural, morphological and magnetic properties for Cu doped nanoscale spinel type ferrites. Journal of Magnetism and Magnetic Materials. 2013;343:86-91.
7. Bleda EA, Yavuz I, Altun Z, Topcu T. High-order-harmonic generation from Rydberg states at fixed Keldysh parameter. Physical Review A - Atomic, Molecular, and Optical Physics. 2013;88(4).
8. Bleda EA, Yavuz I, Altun Z, Trindle C. Computational thermochemistry of glycolaldehyde. International Journal of Quantum Chemistry. 2013;113(8):1147-54.
9. Delice Ö, Kirezli P, Çiftci DK. Higher dimensional cylindrical or Kasner type electrovacuum solutions. General Relativity and Gravitation. 2013;45(11):2251-72.
10. Ermiş E, Çimen Y, Dumludaǧ F, Özkaya AR, Salih B, Bekaroǧlu Ö. Electrochemical and electrical properties of novel mono and ball-type phthalocyanines. Polyhedron. 2013;49(1):129-37.
11. Gülen Y, Bayansal F, Şahin B, Çetinkara HA, Güder HS. Fabrication and characterization of Mn-doped CuO thin films by the SILAR method. Ceramics International. 2013;39(6):6475-80.
12. Kaki E, Özkaya AR, Altindal A, Salih B, Bekaroǧlu Ö. Synthesis, characterization, electrochemistry and VOC sensing properties of novel metallophthalocyanines with four cyclohexyl-phenoxyphthalonitrile groups. Sensors and Actuators, B: Chemical. 2013;188:1033-42.
13. Madakbaş S, Çakmakçi E, Kahraman MV, Esmer K. Preparation, characterisation, and dielectric properties of polypyrrole-clay composites. Chemical Papers. 2013;67(8):1048-53.
14. Mahmood S, Orban I, Ali S, Glans P, Bleda EA, Altun Z, et al. Recombination rate coefficients of boron-like Ne. Astrophysical Journal. 2013;771(2).
15. Oruc I, Akkoyunlu BO, Erdogan I, editors. Investigation of wet, bulk, and dry deposition concentrations in Kirklareli, Turkey. International Multidisciplinary Scientific GeoConference Surveying Geology and Mining Ecology Management, SGEM; 2013.
16. Oruc I, Akkoyunlu BO, Erdogan I, editors. Chemical composition of wet, bulk, and dry deposition in kirklareli, Turkey. International Multidisciplinary Scientific GeoConference Surveying Geology and Mining Ecology Management, SGEM; 2013.
17. Sipahioǧlu S, Madakbaş S, Arda L, Esmer K. Structural and Dielectric Properties of Two Different BaTiO3/Polyaniline Nanocomposites. Journal of Inorganic and Organometallic Polymers and Materials. 2013;23(2):333-9.

18. Taşcioǧlu S, Yalçin B, Dumludaǧ F, Kaki E. Synthesis in water-free DMF, characterization, electrical, and gas sensing properties of bis[2-(2-aminoethylamino)ethanol]copper(II) dibromide. Chemical Papers. 2013;67(6):613-23. 19. Trindle C, Bleda EA, Altun Z. Structure and energetics of cyclopropane carboxaldehyde. International Journal of Quantum Chemistry. 2013;113(8):1155-61.

20. Unal H, Esmer K, Mimaroglu A. Mechanical, electrical and tribological properties of graphite filled polyamide-6 composite materials. Journal of Polymer Engineering. 2013;33(4):351-5.

21. Yaraşir MN, Kandaz M, Akyildiz A, Karadeniz K, Dumludaǧ F, Koca A. Vic-dioxime complexes bearing carboxyester and picolyl amide functionality: Synthesis, characterization, spectroscopy, electrochemistry, and electrical properties. Monatshefte fur Chemie. 2013;144(7):951-62.

22. Yavuz I. Gas population effects in harmonic emission by plasmonic fields. Physical Review A - Atomic, Molecular, and Optical Physics. 2013;87(5).  

 
2012 

1. Alevli M, Ozgit C, Donmez I, Biyikli N. Optical properties of AlN thin films grown by plasma enhanced atomic layer deposition. Journal of Vacuum Science and Technology A: Vacuum, Surfaces and Films. 2012;30(2).
2. Ali S, Orban I, Mahmood S, Altun Z, Glans P, Schuch R. Electron-ion recombination rate coefficients for C II forming CI. Astrophysical Journal. 2012;753(2).
3. Alikma F, Birlikseven C, Gulmez G, Turhan E, Coker EG, Topal U. Improving the sensitivity of superconductor-based dc magnetometer. Journal of Superconductivity and Novel Magnetism. 2012;25(7):2539-45.
4. Alkis S, Alevli M, Burzhuev S, Vural HA, Okyay AK, Ortaç B. Generation of InN nanocrystals in organic solution through laser ablation of high pressure chemical vapor deposition-grown InN thin film. Journal of Nanoparticle Research. 2012;14(8).
5. Bayrak R, Karaoglu K, Ünver Y, Sancak K, Dumludag F, Degirmencioglu I. Synthesis, characterization, spectral and electrical properties of peripherally tetratriazole-substituted phthalocyanines and its metal complexes. Journal of Organometallic Chemistry. 2012;712:57-66.
6. Bleda EA, Yumak A, Yavuz I, Altun Z. Dielectronic recombination in He-like, Li-like and be-like bismuth and KLM resonances. Journal of Physics: Conference Series. 2012;388(PART 6).
7. Intepe A, Kazan S, Chetry KB, Mikailzade F, Yilgin R, Aktas B, et al. Magnetic resonance studies of half-metallic epitaxial CrO2 thin films grown on differently oriented TiO2 substrates. Journal of Superconductivity and Novel Magnetism. 2012;25(8):2647-51.
8. Kizilkaya C, Dumludaǧ F, Karataş S, Apohan NK, Altindal A, Güngör A. The effect of titania content on the physical properties of polyimide/titania nanohybrid films. Journal of Applied Polymer Science. 2012;125(5):3802-10.
9. Klie RF, Qiao Q, Paulauskas T, Gulec A, Rebola A, Öǧüt S, et al. Observations of Co4 + in a higher spin state and the increase in the seebeck coefficient of thermoelectric Ca 3Co 4O 9. Physical Review Letters. 2012;108(19).
10. Leavens BBH, Trindle CO, Sabat M, Altun Z, Demas JN, DeGraff BA. Photophysical and analyte sensing properties of cyclometalated Ir(III) complexes. Journal of Fluorescence. 2012;22(1):163-74.
11. Odabaş Z, Orman EB, Durmuş M, Dumludag F, Özkaya AR, Bulut M. Novel alpha-7-oxy-4-(4-methoxyphenyl)-8-methylcoumarin substituted metal-free, Co(II) and Zn(II) phthalocyanines: Photochemistry, photophysics, conductance and electrochemistry. Dyes and Pigments. 2012;95(3):540-52.
12. Oguz K, Ozdemir M, Dur O, Coey JMD. Low magnetisation alloys for in-plane spin transfer torque devices. Journal of Applied Physics. 2012;111(11).
13. Salan U, Altindal A, Özkaya AR, Salih B, Bekaroǧlu O. Photovoltaic and electrocatalytic properties of novel ball-type phthalocyanines bridged with four dicumarol. Dalton Transactions. 2012;41(17):5177-87.
14. Şengül A, Dogan HZ, Altindal A, Özkaya AR, Salih B, Bekaroglu Ö. Synthesis, interface (Au/M 2Pc 2/p-Si), electrochemical and electrocatalytic properties of novel ball-type phthalocyanines. Dalton Transactions. 2012;41(25):7559-72.
15. Topal U, Alikma F. The 2nd harmonic signal analysis in Ca-doped Y-123 superconductors: Sensing DC-fields down to 0.5 nT. Sensors and Actuators, A: Physical. 2012;183:43-9.
16. Topal U, Alikma F, Birlikseven C, Uzun O, Kölemen U. Measurements of ultra-low DC fields by high-T c superconducting cores: The effect of calcination temperature. Journal of Alloys and Compounds. 2012;530:91-6.
17. Yabaş E, Sülü M, Dumludag F, Özkaya AR, Salih B, Bekaroglu Ö. Electrical and electrochemical properties of double-decker Lu(III) and Eu(III) phthalocyanines with four imidazoles and N-alkylated imidazoles. Polyhedron. 2012;42(1):195-205.
18. Yavuz I. Generation of a broadband xuv continuum in high-order-harmonic generation by spatially inhomogeneous fields. Physical Review A - Atomic, Molecular, and Optical Physics. 2012;85(1).
19. Yavuz I, Altun Z, Topcu T. Wavelength scaling of high-order-harmonic-generation efficiency by few-cycle laser pulses: Influence of carrier-envelope phase. Physical Review A - Atomic, Molecular, and Optical Physics. 2012;86(4).
20. Yavuz I, Bleda E, Altun Z. Stochastic enhancement of high-order harmonic generation. Journal of Physics: Conference Series. 2012;388(PART 3).
21. Yavuz I, Yumak A, Bleda EA, Altun Z. Dielectronic recombination in he-like, Li-like and be-like iodine and KLM resonances. Journal of Physics: Conference Series. 2012;388(PART 6).
22. Yilgin R, Yurtisigi MK, Parabas A, Turksoy M, Ozdemir M, Aktas B, et al. Ferromagnetic behavior of Fe+ implanted si(100) semiconductor. Journal of Superconductivity and Novel Magnetism. 2012;25(8):2731-5.
23. Yumak A, Karakaş V, Altun Z. Dielectronic recombination in he-like, Li-like and be-like yttrium and KLM resonances. Journal of Physics: Conference Series. 2012;388(PART 6).

2011

1.Agirtas, M. S., A. Altindal, B. Salih, S. Saydam, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical and Electrical Properties of Novel Mono and Ball-Type Metallophthalocyanines with Four 9,9-Bis(4-Hydroxyphenyl)Fluorene." Dalton Transactions 40, no. 13 (2011): 3315-3324.
2.Akdogan, N., S. Kazan, B. Aktas, M. Ozdemir, H. Inam, M. Obaida, J. Dudek, and K. Westerholt. "Field Cooling-Induced Magnetic Anisotropy in Exchange Biased Coo/Fe Bilayer Studied by Ferromagnetic Resonance." Journal of Magnetism and Magnetic Materials 323, no. 3-4 (2011): 346-350.
3.Alevli, M., C. Ozgit, and I. Donmez. "The Influence of Growth Temperature on the Properties of Aln Films Grown by Atomic Layer Deposition." Acta Physica Polonica A 120, no. 6A (2011): A58-A60.
4.Baykal, A., and O. Delice. "A Unified Approach to Variational Derivatives of Modified Gravitational Actions." Classical and Quantum Gravity 28, no. 1 (2011).
5.Boyraz, C., D. Mazumdar, M. Iliev, V. Marinova, J. X. Ma, G. Srinivasan, and A. Gupta. "Structural and Magnetic Properties of Lithium Ferrite (Life5o8) Thin Films: Influence of Substrate on the Octahedral Site Order." Applied Physics Letters 98, no. 1 (2011).
6.Elmali, D., A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Synthesis and Characterization, Novel across Adjacent Ring Formed Phthalocyanine." Dalton Transactions 40, no. 3 (2011): 651-660.
7.Erdem, M., G. Ozen, and C. Tav. "Crystallization Behaviour of Neodymium Doped Yttrium Silicate Nanophosphors." Journal of the European Ceramic Society 31, no. 14 (2011): 2629-2631.
8.Erkovan, M., S. T. Ozturk, R. Topkaya, M. Ozdemir, B. Aktas, and O. Ozturk. "Ferromagnetic Resonance Investigation of Py/Cr Multilayer System." Journal of Applied Physics 110, no. 2 (2011).
9.Gumrukcu, G., M. U. Ozgur, A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Synthesis and Electrochemical, Electrical and Gas Sensing Properties of Novel Mononuclear Metal-Free, Zn(Ii), Ni(Ii), Co(Ii), Cu(Ii), Lu(Iii) and Double-Decker Lu(Iii) Phthalocyanines Substituted with 2-(2h-1,2,3-Benzotriazol-2-Yl)-4-(1,1,3,3-Tetramethylbutyl) Phenoxy." Synthetic Metals 161, no. 1-2 (2011): 112-123.
10.Kaya, A. U., K. Esmer, N. Tekin, and S. K. Beyaz. "Investigation of Temperature, Thermodynamic Parameters and Dielectrical Properties of Poly(Vinylimidazole)-Na-Bentonite Nanocomposite." Journal of Applied Polymer Science 120, no. 2 (2011): 874-879.
11.Mergen, A., H. Zorlu, M. Ozdemir, and M. Yumak. "Dielectric Properties of Sm, Nd and Fe Doped Bi1.5zn0.92nb1.5o6.92 Pyrochlores." Ceramics International 37, no. 1 (2011): 37-42.
12.Mergen, A., H. Zorlu, M. Ozdemir, and M. Yumak.. "Fabrication and Characterisation of Cr and Co Doped Bi1.5zn0.92nb1.5o6.92 Pyrochlores." Journal of the European Ceramic Society 31, no. 14 (2011): 2633-2639.
13.Odabas, Z., A. Altindal, and M. Bulut. "Synthesis, Characterization and Electrical Properties of Novel Metal-Free, Co(Ii), Cu(Ii), Fe(Ii), Mn(Ii), Sn(Ii) Phthalocyanines Peripherally Tetra-Substituted with 2,3-Dihydro-1h-Inden-5-Yloxy Moiety." Synthetic Metals 161, no. 15-16 (2011): 1742-1752.
14.Okay, C., B. Z. Rameev, S. Guler, R. I. Khaibullin, R. R. Khakimova, Y. N. Osin, N. Akdogan, A. I. Gumarov, A. Nefedov, H. Zabel, and B. Aktas. "Optical and Magnetic Properties of Ni-Implanted and Post-Annealed Zno Thin Films." Applied Physics a-Materials Science & Processing 104, no. 2 (2011): 667-675.
15.Qiao, Q., A. Gulec, T. Paulauskas, S. Kolesnik, B. Dabrowski, M. Ozdemir, C. Boyraz, D. Mazumdar, A. Gupta, and R. F. Klie. "Effect of Substrate on the Atomic Structure and Physical Properties of Thermoelectric Ca3co4o9 Thin Films." Journal of Physics-Condensed Matter 23, no. 30 (2011).
16.Sen, P., F. Dumludag, B. Salih, A. R. Ozkaya, and O. Bekaroglu. "Synthesis and Electrochemical, Electrochromic and Electrical Properties of Novel S-Triazine Bridged Trinuclear Zn(Ii), Cu(Ii) and Lu(Iii) and a Tris Double-Decker Lu(Iii) Phthalocyanines." Synthetic Metals 161, no. 13-14 (2011): 1245-1254.
17.Tav, C., and S. Yilmazturk. "Temperature and Weight Dependence of Free Volumes in Conducting Composite Polymer Using Positron Annihilation Techniques." High Temperature Materials and Processes 30, no. 1-2 (2011): 193-198.
18.Yabas, E., M. Sulu, S. Saydam, F. Dumludag, B. Salih, and O. Bekaroglu. "Synthesis, Characterization and Investigation of Electrical and Electrochemical Properties of Imidazole Substituted Phthalocyanines." Inorganica Chimica Acta 365, no. 1 (2011): 340-348.
19.Yavuz, I., Z. Altun, and T. Topcu. "Enhancement of High-Order Harmonic Generation in the Presence of Noise." Journal of Physics B-Atomic Molecular and Optical Physics 44, no. 13 (2011).
20.Yavuz, I., and G. A. A. Ciftcioglu. "Dft Characterization of the First Step of Methyl Acrylate Polymerization: Performance of Modern Functionals in the Complete Basis Limit." Computational and Theoretical Chemistry 978, no. 1-3 (2011): 88-97.

2010

1.Akdeniz, G., U. Yahsi, and C. Tav. "Viscous Behavior of Ps, Pp, and Abs in Terms of Temperature and Pressure-Dependent Hole Fraction." Journal of Applied Polymer Science 117, no. 1 (2010): 110-113.
2.Aktas, S., and O. Gazioglu. "Monte Carlo Simulation of Three Dimensional Pancake Model with Point-Like and Columnar Pinning Centers." Physica B-Condensed Matter 405, no. 2 (2010): 678-681.
3.Bayrakdar, H., and K. Esmer. "Dielectric Characterization of Nixco1-Xfe2o4 Nanocrystals Thin Film over a Broad Frequency Range (1 Mhz-3 Ghz)." Journal of Applied Physics 107, no. 4 (2010).
4.Ceyhan, T., A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Novel Ball-Type Four Dithioerythritol Bridged Metallophthalocyanines and Their Water-Soluble Derivatives: Synthesis and Characterization, and Electrochemical, Electrocatalytic, Electrical and Gas Sensing Properties." Dalton Transactions 39, no. 41 (2010): 9801-9814.
5.Ciftcioglu, G. A., C. Trindle, and I. Yavuz. "Focal Point Analysis of Torsional Isomers of Acrylic Acid." Molecular Physics 108, no. 19-20 (2010): 2601-2609.
6.Kandaz, M., A. T. Bilgicli, and A. Altindal. "Metal Ion Sensing Functional Mono and Double-Decker Lanthanide Phthalocyanines: Synthesis, Characterization and Electrical Properties." Synthetic Metals 160, no. 1-2 (2010): 52-60.
7.Kazan, S., F. A. Mikailzade, M. Ozdemir, B. Aktas, B. Rameev, A. Intepe, and A. Gupta. "Ferromagnetic Resonance in Double Perovskite Epitaxial Thin Films of La2nimno6 on Srtio3 and Ndgao3 Substrates." Applied Physics Letters 97, no. 7 (2010).
8.Madakbas, S., K. Esmer, E. Kayahan, and M. Yumak. "Synthesis and Dielectric Properties of Poly(Aniline)/Na-Bentonite Nanocomposite." Science and Engineering of Composite Materials 17, no. 3 (2010): 145-153.
9.Madakbas, S., K. Esmer, and M. H. Ugur. "Thermal and Electrochemical Behaviour of Na/Bentonite-Polyaniline Nanocomposite in Different Media." High Temperature Materials and Processes 29, no. 4 (2010): 269-276.
10.Odabas, Z., A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Novel Ball-Type Homo- and Hetero-Dinuclear Phthalocyanines with Four 1,1 '-Methylenedinaphthalen-2-Ol Bridges: Synthesis and Characterization, Electrical and Gas Sensing Properties and Electrocatalytic Performance Towards Oxygen Reduction." Sensors and Actuators B-Chemical 145, no. 1 (2010): 355-366.
11.Odabas, Z., F. Dumludag, A. R. Ozkaya, S. Yamauchi, N. Kobayashi, and O. Bekaroglu. "Novel Homo- and Heterobinuclear Ball-Type Phthalocyanines: Synthesis and Electrochemical, Electrical, Epr and Mcd Spectral Properties." Dalton Transactions 39, no. 35 (2010): 8143-8152.
12.Odabas, Z., I. Koc, A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Synthesis and Electrochemical, in Situ Spectroelectrochemical, Electrical and Gas Sensing Properties of Ball-Type Homo- and Hetero-Dinuclear Phthalocyanines with Four 1a,8b-Dihydronaphtho B Naphthofuro 3,2-D Furan-7,10-Diyl Bridges." Synthetic Metals 160, no. 9-10 (2010): 967-977.
13.Oner, Y., M. Ozdemir, S. Kazan, A. C. Basaran, B. Aktas, and T. Sato. "Exchange Bias in Pt Doped Nimn Thick Films." Journal of Applied Physics 107, no. 9 (2010).
14.Topkaya, R., M. Erkovan, A. Ozturk, O. Ozturk, B. Aktas, and M. Ozdemir. "Ferromagnetic Resonance Studies of Exchange Coupled Ultrathin Py/Cr/Py Trilayers." Journal of Applied Physics 108, no. 2 (2010).
15.Yumak, A., I. Yavuz, Z. Altun, and C. Trindle. "Two Small Thermodynamically Stable Organic Dications." Journal of Molecular Structure-Theochem 940, no. 1-3 (2010): 6-12.

2009 

1.Ataoglu, S., L. Arda, N. Kadioglu, O. Cakiroglu, O. Bulut, A. N. Gulluoglu, and I. Belenli. "Preparation and Thermal Stress Analysis of Al2o3 Insulation Coatings on Ss-304 Tape." Ieee Transactions on Applied Superconductivity 19, no. 3 (2009): 2375-2378.
2.Ceyhan, T., A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Synthesis, Characterization, and Electrocatalytic and Electrical Properties of Novel Ball-Type Four Cyclopentyldisilanoxy-Poss Bridged Metallophthalocyanines." Dalton Transactions, no. 46 (2009): 10318-10329.
3.Demirel, E., M. Ozdemir, and B. Aktas. "Negative Refractive Index Ferromagnetic Materials with Negative Permeability at Zero Applied Magnetic Field." Applied Magnetic Resonance 36, no. 1 (2009): 69-80.
4.Esmer, K., and E. Kayahan. "Influence of Alkali Metallization (Li, Na and K) on Photoluminescence Properties of Porous Silicon." Applied Surface Science 256, no. 5 (2009): 1548-1552.
5.Oner, Y., M. Ozdemir, A. C. Basaran, B. Aktas, and T. Sato. "Long Range Magnetic Ordering with Giant Magnetic Moments in Pt Doped Nimn Thin Films." Journal of Applied Physics 105, no. 7 (2009).
6.Orban, I., Z. Altun, A. Kallberg, A. Simonsson, G. Andler, A. Paal, M. Blom, P. Lofgren, S. Trotsenko, S. Bohm, and R. Schuch. "Experimental Dielectronic Recombination Rate Coefficients for Na-Like S Vi and Na-Like Ar Viii." Astronomy & Astrophysics 498, no. 3 (2009): 909-914.
7.Ozer, M., A. Altindal, A. R. Ozkaya, and O. Bekaroglu. "Ball-Type Supramolecular Metallophthalocyanines with Eight Perfluorodecyl Units: Chemosensors for So2 and Electrocatalysts for Oxygen Reduction." Dalton Transactions, no. 17 (2009): 3175-3181.
8.Qureshi, A., A. Atindal, and A. Mergen. "Electrical and Gas Sensing Properties of Li and Ti Codoped Nio/Pvdf Thin Film." Sensors and Actuators B-Chemical 138, no. 1 (2009): 71-75.
9.Qureshi, A., A. Mergen, and A. Altindal. "Preparation and Characterization of Li and Ti Codoped Nio Nanocomposites for Gas Sensors Applications." Sensors and Actuators B-Chemical 135, no. 2 (2009): 537-540.
10.Toplan, H. O., M. Okutan, K. Esmer, Y. Atalay, S. Yuruyen, and E. Tarcan. "Dielectrical Properties of a Novel Porcelain Produced from Natural Clay, Waste Glass and Fly Ash." High Temperature Materials and Processes 28, no. 1-2 (2009): 55-65.
11.Trindle, C., and Z. Altun. "Circular Dichroism of Some High-Symmetry Chiral Molecules: B3lyp and Saop Calculations." Theoretical Chemistry Accounts 122, no. 3-4 (2009): 145-155.

2008 

1.Altun, S., A. Altindal, A. R. Ozkaya, M. Bulut, and O. Bekaroglu. "Synthesis, Characterization, Electrochemical and Co(2) Sensing Properties of Novel Mono and Ball-Type Phthalocyanines with Four Phenolphthalein Units." Tetrahedron Letters 49, no. 29-30 (2008): 4483-4486.
2.Altun, Z., A. Yumak, U. Golcek, S. D. Loch, M. S. Pindzola, and D. C. Griffin. "Electron-Impact Ionization of Atomic Ions in the Na Isoelectronic Sequence." Physica Scripta 78, no. 2 (2008).
3.Budak, S., F. Yildiz, M. Ozdemir, and B. Aktas. "Effect of Temperature on the Magnetic Properties of Fe(3)O(4) Thin Films Studied by Ferromagnetic Resonance (Fmr)." Physica Status Solidi B-Basic Solid State Physics 245, no. 8 (2008): 1647-1652.
4.Cakiroglu, O., L. Arda, C. Boyraz, and O. A. Sacli. "Electrical Characterizations of Mgo-Zro2 High Temperature Sol-Gel Insulations Coatings on Different Types of Epoxies." Ieee Transactions on Applied Superconductivity 18, no. 2 (2008): 1398-1401.
5.Canlica, M., A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical, and Electrical Measurements of Novel 4,4 '-Isopropylidendioxydiphenyl Bridged Bis and Cofacial Bis-Metallophthalocyanines (Zn, Co)." Polyhedron 27, no. 7 (2008): 1883-1890.
6.Elagoz, S., P. Baser, and U. Yahsi. "The Magnetic Field Dependency of Hydrogenic Impurity Binding Energy under Inverse Lateral Parabolic Potential." Physica B-Condensed Matter 403, no. 21-22 (2008): 3879-3882.
7.Ozer, M., A. Altindal, B. Salih, M. Bulut, and O. Bekaroglu. "Synthesis and Characterization of Novel Cofacial Bis-Phthalocyanines Containing 16-Crown-5 Ether Groups." Tetrahedron Letters 49, no. 5 (2008): 896-900.
8.Tasaltin, N., F. Dumludag, M. A. Ebeoglu, H. Yuzer, and Z. Z. Ozturk. "Pd/Native Nitride/N-Gaas Structures as Hydrogen Sensors." Sensors and Actuators B-Chemical 130, no. 1 (2008): 59-64.
9.Yahsi, U., K. Ulutas, C. Tav, and D. Deger. "On the Ionic Conductivity of Polymer Electrolytes in Terms of Hole Fraction." Journal of Polymer Science Part B-Polymer Physics 46, no. 20 (2008): 2249-2254.
10.Yavuz, I., and C. Trindle. "Structure, Binding Energies, and Ir-Spectral Fingerprinting of Formic Acid Dimers." Journal of Chemical Theory and Computation 4, no. 3 (2008): 533-541.

2007 

1.Altun, Z., A. Yumak, I. Yavuz, N. R. Badnell, S. D. Loch, and M. S. Pindzola. "Dielectronic Recombination Data for Dynamic Finite-Density Plasmas - Xiii. The Magnesium Isoelectronic Sequence." Astronomy & Astrophysics 474, no. 3 (2007): 1051-1059.
2.Aslan, N., E. Onbasioglu, S. Balci, and A. Erdogan. "Parallelizaton of Visual Magneto-Hydrodynamics Code Based on Fluctuation Distribution Scheme on Triangular Grids." Computers & Fluids 36, no. 5 (2007): 961-973.
3.Ceyhan, T., A. Altindal, A. R. Ozkaya, O. Celikbicak, B. Salih, M. K. Erbil, and O. Bekaroglu. "Synthesis, Characterization and Electrochemical Properties of Novel Metal Free and Zinc(Ii) Phthalocyanines of Ball and Clamshell Types." Polyhedron 26, no. 15 (2007): 4239-4249.
4.Ceyhan, T., A. Altindal, A. R. Ozkaya, M. K. Erbil, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical, Electrical and Gas Sensing Properties of a Novel Tert-Butylcalix 4 Arene Bridged Bis Double-Decker Lutetium(Iii) Phthalocyanine." Polyhedron 26, no. 1 (2007): 73-84.
5.Ceyhan, T., A. Altindal, A. R. Ozkaya, B. Salih, M. K. Erbil, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical and Electrical Properties of a Novel Ball-Type Hexanuclear Metallophthalocyanine, Bridged by Calix 4 Arenes Substituted with Four Hexylthiometallophthalocyanines through Nitro Coupling." Journal of Porphyrins and Phthalocyanines 11, no. 9 (2007): 625-634.
6.Kulac, D., M. Bulut, A. Altindal, A. R. Ozkaya, B. Salih, and O. Bekaroglu. "Synthesis and Characterization of Novel 4-Nitro-2-(Octyloxy)Phenoxy Substituted Symmetrical and Unsymmetrical Zn(Ii), Co(Ii) and Lu(Iii) Phthalocyanines." Polyhedron 26, no. 18 (2007): 5432-5440.
7.Odabas, Z., A. Altindal, A. R. Ozkaya, M. Bulut, B. Salih, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical and Electrical Properties of Novel Mononuclear and Binuclear Ball-Type Zn(Ii) Phthalocyanines Substituted with 1a,8b-Dihydronaphtho B Naphthofuro- 3,2-D Furan-7,10-Diyl." Polyhedron 26, no. 14 (2007): 3505-3512.
8.Odabas, Z., A. Altindal, A. R. Ozkaya, M. Bulut, B. Salih, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical, Spectroelectrochemical and Electrical Measurements of Novel Ball-Type Four 1,1 '-Methylenedinaphthalen-2-Ol Bridged Metal-Free, Zinc(Ii) and Cobalt(Ii), and Metal-Free Clamshell Phthalocyanines." Polyhedron 26, no. 3 (2007): 695-707.
9.Odabas, Z., A. Altindal, B. Salih, M. Bulut, and O. Bekaroglu. "Synthesis, Characterization and Electrical Properties of Novel Mono- and Cofacial Bisphthalocyanines Bridged with Four 1a,8b-Dihydronaphtho B Naphthofuro 3,2-D Furan-7,10-Diyl Units." Tetrahedron Letters 48, no. 36 (2007): 6326-6329.
10.Ozer, M., A. Altindal, A. R. Ozkaya, B. Salih, M. Bulut, and O. Bekaroglu. "Synthesis, Characterization, and Electrochemical and Electrical Properties of Novel Pentaerythritol-Bridged Cofacial Bismetallophthalocyanines and Their Water-Soluble Derivatives." European Journal of Inorganic Chemistry, no. 22 (2007): 3519-3526.

 

Alevli, M. and N. Gungor (2018). "Influence of N-2/H-2 and N-2 plasma on binary III-nitride films prepared by hollow-cathode plasma-assisted atomic layer deposition." Journal of Vacuum Science & Technology A 36(1).
    The authors reported the hollow-cathode plasma-assisted atomic layer deposition of AlN, GaN, and InN films using N-2-only and N-2/H-2 plasma. In this study, the authors analyzed the effect of plasma gas composition on the properties of deposited binary III-nitride thin films. Toward this goal, AlN, GaN, and InN films were deposited on Si (100) substrates using N-2-only (50 sccm), as well as N-2/H-2 (50+50, 50+25 sccm) plasma to investigate the impact of H-2 flow. Grazingincidence x-ray diffraction (GIXRD) patterns of AlN and GaN thin films deposited with N-2/H-2 plasma remained almost unchanged when H-2 flow decreased from 50 to 25 sccm. On the other hand, the use of N-2 plasma without any H-2 resulted in amorphous GaN thin films with significant carbon impurity within the bulk film. In the case of AlN, similar behavior was observed as the crystal structure is significantly altered to amorphouslike material. Thicknesses of AlN and GaN thin films increased tremendously when N-2-only was used as the plasma gas. Furthermore, refractive index values of both AlN and GaN films decreased upon the use of N-2-only plasma, which confirm the deterioration of the film quality. Structural weaknesses of GaN and AlN films deposited with N-2-only plasma are due to presences of carbon impurities that are trapped inside the growing film. Interestingly, the authors did not observe similar results in InN films grown with N-2/H-2 plasma. For InN, GIXRD and spectroscopic ellipsometry results show that the phases of deposited films change from InN to In+InN as H-2 content in the plasma gas is increased. On the other hand, InN films grown with N-2-only plasma show improved structural properties. However, significantly higher N-2 plasma exposure times are needed to minimize the residual carbon content in deposited InN layers. Published by the AVS.

Baltaci, H., et al. (2018). "An Extreme Hailstorm on 27 July 2017 in Istanbul, Turkey: Synoptic Scale Circulation and Thermodynamic Evaluation." Pure and Applied Geophysics 175(11): 3727-3740.
    During the afternoon hours of July 27, 2017, an extreme hailstorm struck the most populated city of Turkey, Istanbul. This rapidly growing supercell which produces large hail led to numerous injuries and damaged automobiles, houses, aircrafts, crops, and infrastructure of the city. As a result of the movement of the cut-off cyclone from Middle East to western Turkey, warm air advection penetrated over Marmara, and the land surface temperature of Istanbul reached 34 degrees C (5 degrees C above the mean). The transport of significant amount of moisture, which was caused by excessive heating of Marmara Sea surface temperatures (24.9 degrees C), to the low levels of the atmosphere by strong southwesterly winds enabled the increase of low-level moisture convergence. Both abnormal temperature differences between land and 500-hPa level (41.5 degrees C) and excessive wind shear values (20.3m/s) between surface and 6km above ground level (AGL) increased the thermal instability and updraft conditions of the baroclinic atmosphere. This condition resulted in thunderstorms, stormy and gale wind gusts (31.9m/s 15:20 UTC), extreme lightning activity (totally 2696 cloud-to-ground and 5791 intracloud), large hailstones between 3-6cm diameter and high hourly precipitation amounts (38.7, 36.2, 29.8, and 27.2mm in Sisli, Kadikoy, Uskudar, and Fatih regions, respectively, between 14:00 and 15:00 UTC) in the urban settlements of the city. The stability indices, Showalter, K, Total of totals, SWEAT, and CAPE also showed the high probability of severe thunderstorm occurrence over Istanbul. Based on a comparison among these five indices, the SWEAT index is most appropriate to represent the atmospheric conditions over the city owing to low-level moisture, warm air advection, and low and mid-level wind speed terms in its equation.

Baltaci, H., et al. (2018). "Relationships between teleconnection patterns and Turkish climatic extremes." Theoretical and Applied Climatology 134(3-4): 1365-1386.
    This is a study on the effects of teleconnection patterns (TPs) on the extremes of temperature and precipitation over Turkey. Relationships between five teleconnection patterns, North Atlantic Oscillation (NAO), Arctic Oscillation (AO), East Atlantic-Western Russia (EAWR), East Atlantic (EA), and Scandinavian (SCA) patterns, and 11 climate extreme indices were studied by using 94 uniformly distributed meteorological stations over Turkey for the period of 1965-2014. Analyzing strong positive and negative temperature deviations from the 50-year-winter means shows that such extremes can often be explained by using AO and EAWR patterns. During the negative AO, generally more warm days occur over Black Sea (r=-0.6) and Aegean regions (r=-0.7). This phase of AO also generates above-normal precipitation in the western parts of the Anatolian Peninsula (r around -0.5). Winter-time negative AO is mainly associated with the presence of a deepened Genoa cyclone over Italy that can transport warm and moist air mass from Mediterranean Sea towards Turkey by strong westerly winds. In contrast, positive EAWR is mainly connected to cold nights over Black Sea (r=0.6) and Aegean regions (r=0.6) together with positive precipitation anomalies at the seaside stations of the eastern Black Sea region. On the other hand, when positive EAWR prevails, Azores high-pressure center expands towards continental Europe bringing cold air by strong northerly winds together with higher moisture transport from the Black Sea. These results could pave the way for new possibilities regarding the projection of extremes in downscaling techniques.

Dumludag, F., et al. (2018). DC and AC conductivity properties of bovine dentine hydroxyapatite (BDHA). 3rd International Conference on Smart Material Research. 293.
    Bovine dentine bio-waste may be used as a potential natural source of hydroxyapatite (BDHA), thus extraction of bovine dentin hydroxyapatite (BDHA) from bio-waste is significantly important to fabricate in a simple, economically and environmentally preferable. DC and AC conductivity properties of BDHA were investigated depending on sintering temperature (1000 degrees C - 1300 degrees C) in air and vacuum ( J/psi Lambda decays from pp collisions at root s=7 and 8 TeV." Physical Review D 97(7).
    An analysis of the bottom baryon decay Lambda(b) -> J/psi(-> mu(+)mu(-))Lambda( -> p pi(-)) is performed to measure the Lambda(b) polarization and three angular parameters in data from pp collisions at root s = 7 and 8 TeV, collected by the CMS experiment at the Large Hadron Collider. The Lambda(b) polarization is measured to be 0.00 +/- 0.06(stat) +/- 0.06(syst) and the parity-violating asymmetry parameter is determined to be 0.14 +/- 0.14(stat) +/- 0.10(syst). The measurements are compared to various theoretical predictions, including those from perturbative quantum chromodynamics.

Sirunyan, A. M., et al. (2018). "Measurement of the Z/gamma* -> tau tau cross section in pp collisions at root s=13 TeV and validation of tau lepton analysis techniques." European Physical Journal C 78(9).
    A measurement is presented of the Z/gamma*->tau tau cross section in pp collisions at root s = 13 TeV, using data recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 2.3 fb(-1). The product of the inclusive cross section and branching fraction is measured to be sigma(pp -> Z/gamma*+X) B(Z/gamma*->tau tau) = 1848 +/- 12 (stat) +/- 67 (syst + lumi) pb, in agreement with the standard model expectation, computed at next-to-next-to-leading order accuracy in perturbative quantum chromodynamics. The measurement is used to validate new analysis techniques relevant for future measurements of tau lepton production. The measurement also provides the reconstruction efficiency and energy scale for tau decays to hadrons + nu(tau) final states, determined with respective relative uncertainties of 2.2 and 0.9%.

Sirunyan, A. M., et al. (2018). "Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
    Measurements of differential t (t) over bar production cross sections are presented in the single-lepton decay channel, as a function of a number of kinematic event variables. The measurements are performed with proton-proton collision data at root s = 13 TeV, collected by the CMS experiment at the LHC during 2016, with an integrated luminosity of 35.9 fb(-1). The data are compared to a variety of state-of-the-art leading-order and next-to-leading order t (t) over bar simulations.

Sirunyan, A. M., et al. (2018). "Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
    Measurements of Higgs boson properties in the H decay channel are reported. The analysis is based on data collected by the CMS experiment in proton-proton collisions at =13 TeV during the 2016 LHC running period, corresponding to an integrated luminosity of 35.9 fb(-1). Allowing the Higgs mass to float, the measurement yields a signal strength relative to the standard model prediction of 1.18-0.14+0.17=1.18-0.11+0.12(stat)-0.07+0.09(syst)-0.06+0.07(theo), which is largely insensitive to the exact Higgs mass around 125 GeV. Signal strengths associated with the different Higgs boson production mechanisms, couplings to bosons and fermions, and effective couplings to photons and gluons are also measured.

Sirunyan, A. M., et al. (2018). "Observation of Medium-Induced Modifications of Jet Fragmentation in Pb-Pb Collisions at root s(NN)=5.02 TeV Using Isolated Photon-Tagged Jets." Physical Review Letters 121(24).
    Measurements of fragmentation functions for jets associated with an isolated photon are presented for the first time in pp and Pb-Pb collisions. The analysis uses data collected with the CMS detector at the CERN LHC at a nucleon-nucleon center-of-mass energy of 5.02 TeV. Fragmentation functions are obtained for jets with P-T(jet) 30 GeV/c in events containing an isolated photon with p(T)(gamma) 60 GeV/c, using charged tracks with transverse momentum p(T)(trk) > 1 GeV/c in a cone around the jet axis. The association with an isolated photon constrains the initial p(T) and azimuthal angle of the parton whose shower produced the jet. For central Pb-Pb collisions, modifications of the jet fragmentation functions are observed when compared to those measured in pp collisions, while no significant differences are found in the 50% most peripheral collisions. Jets in central Pb-Pb events show an excess (depletion) of low (high) p(T) particles, with a transition around 3 GeV/c. This measurement shows for the first time the in-medium shower modifications of partons (quark dominated) with well-defined initial kinematics. It constitutes a new well-controlled reference for testing theoretical models of the parton passage through the quark-gluon plasma.

Sirunyan, A. M., et al. (2018). "Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at root s=13 TeV." Journal of Instrumentation 13.
    The CMS muon detector system, muon reconstruction software, and high-level trigger underwent significant changes in 2013-2014 in preparation for running at higher LHC collision energy and instantaneous luminosity. The performance of the modified system is studied using proton-proton collision data at center-of-mass energy root s = 13 TeV, collected at the LHC in 2015 and 2016. The measured performance parameters, including spatial resolution, efficiency, and timing, are found to meet all design specifications and are well reproduced by simulation. Despite the more challenging running conditions, the modified muon system is found to perform as well as, and in many aspects better than, previously. We dedicate this paper to the memory of Prof. Alberto Benvenuti, whose work was fundamental for the CMS muon detector.

Sirunyan, A. M., et al. (2018). "Search for a heavy resonance decaying into a Z boson and a vector boson in the v(v)over-barq(q)over-bar final state." Journal of High Energy Physics(7).
    A search is presented for a heavy resonance decaying into either a pair of Z bosons or a Z boson and a W boson (ZZ or WZ), with a Z boson decaying into a pair of neutrinos and the other boson decaying hadronically into two collimated quarks that are reconstructed as a highly energetic large-cone jet. The search is performed using the data collected with the CMS detector at the CERN LHC during 2016 in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to a total integrated luminosity of 35.9 fb(-1). No excess is observed in data with regard to background expectations. Results are interpreted in scenarios of physics beyond the standard model. Limits at 95% confidence level on production cross sections are set at 0.9 fb (63 fb) for spin-1 W' bosons, included in the heavy vector triplet model, with mass 4.0 TeV (1.0 TeV), and at 0.5 fb (40 fb) for spin-2 bulk gravitons with mass 4.0 TeV (1.0 TeV). Lower limits are set on the masses of W' bosons in the context of two versions of the heavy vector triplet model of 3.1 TeV and 3.4 TeV, respectively.

Sirunyan, A. M., et al. (2018). "Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2l2q final states at root s=13 TeV." Journal of High Energy Physics(9).
    A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.

Sirunyan, A. M., et al. (2018). "Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets root s at=13 TeV." Journal of High Energy Physics(5).
    A search for a heavy right-handed W boson (W-R) decaying to a heavy right-handed neutrino and a charged lepton in events with two same-flavor leptons (e or mu) and two jets, is presented. The analysis is based on proton-proton collision data, collected by the CMS Collaboration at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb(-1). No significant excess above the standard model expectation is seen in the invariant mass distribution of the dilepton plus dijet system. Assuming that couplings are identical to those of the standard model, and that only one heavy neutrino flavor N-R contributes significantly to the W-R decay width, the region in the two-dimensional (m(WR), m(NR)) mass plane excluded at 95% confidence level extends to approximately m(WR) = 4 : 4TeV and covers a large range of right-handed neutrino masses below the W-R boson mass. This analysis provides the most stringent limits on the W-R mass to date.

Sirunyan, A. M., et al. (2018). "Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
    A search for a new scalar resonance decaying to a pair of Z bosons is performed in the mass range from 130 GeV to 3TeV, and for various width scenarios. The analysis is based on proton-proton collisions recorded by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of 35.9 fb(-1) at a center-of-mass energy of 13TeV. The Z boson pair decays are reconstructed using the 4l, 2l2q, and 2l2 nu final states, where l = e or mu. Both gluon fusion and electroweak production of the scalar resonance are considered, with a free parameter describing their relative cross sections. A dedicated categorization of events, based on the kinematic properties of associated jets, and matrix element techniques are employed for an optimal signal and background separation. A description of the interference between signal and background amplitudes for a resonance of an arbitrary width is included. No significant excess of events with respect to the standard model expectation is observed and limits are set on the product of the cross section for a new scalar boson and the branching fraction for its decay to ZZ for a large range of masses and widths.

Sirunyan, A. M., et al. (2018). "Search for additional neutral MSSM Higgs bosons in the tau tau final state in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(9).
    A search is presented for additional neutral Higgs bosons in the tau tau final state in proton-proton collisions at the LHC. The search is performed in the context of the minimal supersymmetric extension of the standard model (MSSM), using the data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes production of the Higgs boson in association with b quarks. No significant deviation above the expected background is observed. Model-independent limits at 95% confidence level (CL) are set on the product of the branching fraction for the decay into tau leptons and the cross section for the production via gluon fusion or in association with b quarks. These limits range from 18 pb at 90 GeV to 3.5 fb at 3.2 TeV for gluon fusion and from 15 pb (at 90 GeV) to 2.5 fb (at 3.2TeV) for production in association with b quarks, assuming a narrow width resonance. In the m(h)(mod+) scenario these limits translate into a 95% CL exclusion of tan beta > 6 for neutral Higgs boson masses below 250 GeV, where tan beta is the ratio of the vacuum expectation values of the neutral components of the two Higgs doublets. The 95% CL exclusion contour reaches 1.6TeV for tan beta = 60.

Sirunyan, A. M., et al. (2018). "Search for high-mass resonances in dilepton final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
    A search is presented for new high-mass resonances decaying into electron or muon pairs. The search uses proton-proton collision data at a centre-of-mass energy of 13TeV collected by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of 36 fb(-1). Observations are in agreement with standard model expectations. Upper limits on the product of a new resonance production cross section and branching fraction to dileptons are calculated in a model-independent manner. This permits the interpretation of the limits in models predicting a narrow dielectron or dimuon resonance. A scan of different intrinsic width hypotheses is performed. Limits are set on the masses of various hypothetical particles. For the Z(SSM)' (Z(psi)') particle, which arises in the sequential standard model (superstring-inspired model), a lower mass limit of 4.50 (3.90) TeV is set at 95% confidence level. The lightest Kaluza-Klein graviton arising in the Randall-Sundrum model of extra dimensions, with coupling parameters k/(M) over bar (Pl) of 0.01, 0.05, and 0.10, is excluded at 95% con fi dence level below 2.10, 3.65, and 4.25TeV, respectively. In a simpli fi ed model of dark matter production via a vector or axial vector mediator, limits at 95% con fi dence level are obtained on the masses of the dark matter particle and its mediator.

Sirunyan, A. M., et al. (2018). "Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV." Journal of High Energy Physics(6).
    A search for new high-mass resonances in proton-proton collisions having final states with an electron or muon and missing transverse momentum is presented. The analysis uses proton-proton collision data collected in 2016 with the CMS detector at the LHC at a center-of-mass energy of 13TeV, corresponding to an integrated luminosity of 35.9 fb(-1). The transverse mass distribution of the charged lepton-neutrino system is used as the discriminating variable. No significant deviation from the standard model prediction is found. The best limit, from the combination of electron and muon channels, is 5.2TeV at 95% confidence level for the mass of a W' boson with the same couplings as those of the standard model Wboson. Exclusion limits of 2.9TeV are set on the inverse radius of the extra dimension in the framework of split universal extra dimensions. In addition, model-independent limits are set on the production cross section and coupling strength of W' bosons decaying into this final state. An interpretation is also made in the context of an R parity violating supersymmetric model with a slepton as a mediator and flavor violating decay.

Sirunyan, A. M., et al. (2018). "Search for lepton-flavor violating decays of heavy resonances and quantum black holes to e mu final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(4).
    A search is reported for heavy resonances decaying into e mu final states in proton-proton collisions recorded by the CMS experiment at the CERN LHC at root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). The search focuses on resonance masses above 200 GeV. With no evidence found for physics beyond the standard model in the e mu mass spectrum, upper limits are set at 95% confidence level on the product of the cross section and branching fraction for this lepton-flavor violating signal. Based on these results, resonant tau sneutrino production in R-parity violating supersymmetric models is excluded for masses below 1.7 TeV, for couplings lambda(132) = lambda(231) = lambda(311) = 0.01. Heavy Z' gauge bosons with lepton-flavor violating transitions are excluded for masses up to 4.4 TeV. The eit mass spectrum is also interpreted in terms of non-resonant contributions from quantum black-hole production in models with one to six extra spatial dimensions, and lower mass limits are found between 3.6 and 5.6 TeV. In all interpretations used in this analysis, the results of this search improve previous limits by about 1 TeV. These limits correspond to the most sensitive values obtained at colliders.

Sirunyan, A. M., et al. (2018). "Search for narrow and broad dijet resonances in proton-proton collisions at root s=13 TeV and constraints on dark matter mediators and other new particles." Journal of High Energy Physics(8).
    Searches for resonances decaying into pairs of jets are performed using proton-proton collision data collected at root s = 13 TeV corresponding to an integrated luminosity of up to 36 fb(-1). A low-mass search, for resonances with masses between 0.6 and 1.6 TeV, is performed based on events with dijets reconstructed at the trigger level from calorimeter information. A high-mass search, for resonances with masses above 1.6 TeV, is performed using dijets reconstructed offline with a particle-flow algorithm. The dijet mass spectrum is well described by a smooth parameterization and no evidence for the production of new particles is observed. Upper limits at 95% confidence level are reported on the production cross section for narrow resonances with masses above 0.6 TeV. In the context of specific models, the limits exclude string resonances with masses below 7.7 TeV, scalar diquarks below 7.2 TeV, axigluons and colorons below 6.1 TeV, excited quarks below 6.0 TeV, color-octet scalars below 3.4 TeV, W' bosons below 3.3 TeV, Z' bosons below 2.7 TeV, Randall-Sundrum gravitons below 1.8 TeV and in the range 1.9 to 2.5 TeV, and dark matter mediators below 2.6 TeV. The limits on both vector and axial-vector mediators, in a simplified model of interactions between quarks and dark matter particles, are presented as functions of dark matter particle mass and coupling to quarks. Searches are also presented for broad resonances, including for the first time spin-1 resonances with intrinsic widths as large as 30% of the resonance mass. The broad resonance search improves and extends the exclusions of a dark matter mediator to larger values of its mass and coupling to quarks.

Sirunyan, A. M., et al. (2018). "Search for Narrow Resonances in the b-Tagged Dijet Mass Spectrum in Proton-Proton Collisions at root s=8 TeV." Physical Review Letters 120(20).
    A search for narrow resonances decaying to bottom quark-antiquark pairs is presented, using a data sample of proton-proton collisions at root s = 8 TeV corresponding to an integrated luminosity of 19.7 fb(-1). The search is extended to masses lower than those reached in typical searches for resonances decaying into jet pairs at the LHC, by taking advantage of triggers that identify jets originating from bottom quarks. No significant excess of events is observed above the background predictions. Limits are set on the product of cross section and branching fraction to bottom quarks for spin 0, 1, and 2 resonances in the mass range of 325-1200 GeV. These results improve on the limits for resonances decaying into jet pairs in the 325-500 GeV mass range.

Sirunyan, A. M., et al. (2018). "Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models." European Physical Journal C 78(9).
    search is presented for physics beyond the standard model, based on measurements of dijet angular distributions in proton-proton collisions at root s = 13 TeV. The data collected with the CMS detector at the LHC correspond to an integrated luminosity of 35.9 fb(-1). The observed distributions, corrected to particle level, are found to be in agreement with predictions from perturbative quantum chromodynamics that include electroweak corrections. Constraints are placed on models containing quark contact interactions, extra spatial dimensions, quantum black holes, or dark matter, using the detector-level distributions. In a benchmark model where only left-handed quarks participate, contact interactions are excluded at the 95% confidence level up to a scale of 12.8 or 17.5 TeV, for destructive or constructive interference, respectively. The most stringent lower limits to date are set on the ultraviolet cutoff in the Arkani-Hamed-Dimopoulos-Dvali model of extra dimensions. In the Giudice-Rattazzi-Wells convention, the cutoff scale is excluded up to 10.1 TeV. The production of quantum black holes is excluded for masses below 5.9 and 8.2 TeV, depending on the model. For the first time, lower limits between 2.0 and 4.6 TeV are set on the mass of a dark matter mediator for (axial-)vector mediators, for the universal quark coupling g(q) = 1.0.

Sirunyan, A. M., et al. (2018). "Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at root s=13 TeV." Physics Letters B 782: 440-467.
    A search is presented for new physics in events with two low-momentum, oppositely charged leptons (electrons or muons) and missing transverse momentum in proton-proton collisions at a centre-of-mass energy of 13TeV. The data collected using the CMS detector at the LHC correspond to an integrated luminosity of 35.9 fb(-1). The observed event yields are consistent with the expectations from the standard model. The results are interpreted in terms of pair production of charginos and neutralinos ((chi) over tilde (+/-)(1) and (chi) over tilde (0)(2)) with nearly degenerate masses, as expected in natural supersymmetry models with light higgsinos, as well as in terms of the pair production of top squarks ((t) over tilde), when the lightest neutralino and the top squark have similar masses. At 95% confidence level, wino-like (chi) over tilde (+/-)(1)/(chi) over tilde (0)(2) masses are excluded up to 230GeVfor a mass difference of 20GeV relative to the lightest neutralino. In the higgsino-like model, masses are excluded up to 168GeV for the same mass difference. For (t) over tilde pair production, top squark masses up to 450GeVare excluded for a mass difference of 40GeV relative to the lightest neutralino. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for new physics in final states with an energetic jet or a hadronically decaying W or Z boson and transverse momentum imbalance at root s=13 TeV." Physical Review D 97(9).
    A search for new physics using events containing an imbalance in transverse momentum and one or more energetic jets arising from initial-state radiation or the hadronic decay of W or Z bosons is presented. A data sample of proton-proton collisions at root s = 13 TeV, collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 35.9 fb(-1), is used. The observed data are found to be in agreement with the expectation from standard model processes. The results are interpreted as limits on the dark matter production cross section in simplified models with vector, axial-vector, scalar, and pseudoscalar mediators. Interpretations in the context of fermion portal and nonthermal dark matter models are also provided. In addition, the results are interpreted in terms of invisible decays of the Higgs boson and set stringent limits on the fundamental Planck scale in the Arkani-Hamed, Dimopoulos, and Dvali model with large extra spatial dimensions.

Sirunyan, A. M., et al. (2018). "Search for pair production of excited top quarks in the lepton plus jets final state The CMS Collaboration." Physics Letters B 778: 349-370.
    A search is performed for the pair production of spin-3/2 excited top quarks, each decaying to a top quark and a gluon. The search uses the data collected with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). Events are selected by requiring an isolated muon or electron, an imbalance in the transverse momentum, and at least six jets of which exactly two must be compatible with originating from the fragmentation of a bottom quark. No significant excess over the standard model predictions is found. A lower limit of 1.2 TeV is set at 95% confidence level on the mass of the spin-3/2 excited top quark in an extension of the Randall-Sundrum model, assuming a 100% branching fraction of its decay into a top quark and a gluon. These are the best limits to date in a search for excited top quarks and the first at 13 TeV. (c) 2018 The Author(s). Published by Elsevier B. V.

Sirunyan, A. M., et al. (2018). "Search for Physics Beyond the Standard Model in Events with High-Momentum Higgs Bosons and Missing Transverse Momentum in Proton-Proton Collisions at 13 TeV." Physical Review Letters 120(24).
    A search for physics beyond the standard model in events with one or more high-momentum Higgs bosons, H, decaying to pairs of b quarks in association with missing transverse momentum is presented. The data, corresponding to an integrated luminosity of 35.9 fb(-1), were collected with the CMS detector at the LHC in proton-proton collisions at the center-of-mass energy root s = 13 TeV. The analysis utilizes a new b quark tagging technique based on jet substructure to identify jets from H -> b (b) over bar. Events are categorized by the multiplicity of H-tagged jets, jet mass, and the missing transverse momentum. No significant deviation from standard model expectations is observed. In the context of supersymmetry (SUSY), limits on the cross sections of pair-produced gluinos are set, assuming that gluinos decay to quark pairs, H (or Z), and the lightest SUSY particle, LSP, through an intermediate next-to-lightest SUSY particle, NLSP. With large mass splitting between the NLSP and LSP, and 100% NLSP branching fraction to H, the lower limit on the gluino mass is found to be 2010 GeV.

Sirunyan, A. M., et al. (2018). "Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV." Journal of High Energy Physics(8).
    A search for a narrow-width resonance decaying into two Higgs bosons, each decaying into a bottom quark-antiquark pair, is presented. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 35.9 fb(-1) at root s = 13 TeV recorded by the CMS detector at the LHC. No evidence for such a signal is observed. Upper limits are set on the product of the production cross section for the resonance and the branching fraction for the selected decay mode in the resonance mass range from 260 to 1200 GeV.

Sirunyan, A. M., et al. (2018). "Search for R-parity violating supersymmetry in pp collisions at root s=13 TeV using bjets in a final state with a single lepton, many jets, and high sum of large-radius jet masses." Physics Letters B 783: 114-139.
    Results are reported from a search for physics beyond the standard model in proton-proton collisions at a center-of-mass energy of root s=13TeV. The search uses a signature of a single lepton, large jet and bottom quark jet multiplicities, and high sum of large-radius jet masses, without any requirement on the missing transverse momentum in an event. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) recorded by the CMS experiment at the LHC. No significant excess beyond the prediction from standard model processes is observed. The results are interpreted in terms of upper limits on the production cross section for R-parity violating supersymmetric extensions of the standard model using a benchmark model of gluino pair production, in which each gluino decays promptly via (g) over tilde -> tbs. Gluinos with a mass below 1610 GeV are excluded at 95% confidence level. (c) 2018 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP(3).

Sirunyan, A. M., et al. (2018). "Search for single production of vector-like quarks decaying to a b quark and a Higgs boson." Journal of High Energy Physics(6).
    A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted b (b) over bar pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). The data are consistent with background expectations, and upper limits at 95% confidence level on the product of the B quark cross section and the branching fraction are obtained in the range 1.28-0.07 pb, for a narrow B quark with a mass between 700 and 1800 GeV. The production of B quarks with widths of 10, 20 and 30% of the resonance mass is also considered, and the sensitivities obtained are similar to those achieved in the narrow width case. This is the first search at the CERN LHC for the single production of a B quark through its fully hadronic decay channel, and the first study considering finite resonance widths of the B quark.

Sirunyan, A. M., et al. (2018). "Search for standard model production of four top quarks with same-sign and multilepton final states in proton-proton collisions at root s=13TeV." European Physical Journal C 78(2).
    A search for standard model production of four top quarks (t (t) over bart (t) over bar) is reported using events containing at least three leptons (e, mu) or a same-sign lepton pair. The events are produced in proton-proton collisions at a center-of-mass energy of 13 TeVat the LHC, and the data sample, recorded in 2016, corresponds to an integrated luminosity of 35.9 fb(-1). Jet multiplicity and flavor are used to enhance signal sensitivity, and dedicated control regions are used to constrain the dominant backgrounds. The observed and expected signal significances are, respectively, 1.6 and 1.0 standard deviations, and the t (t) over bart (t) over bar cross section ismeasured to be 16.9(-11.4)(+13.8) fb, in agreement with next-to-leading-order standard model predictions. These results are also used to constrain the Yukawa coupling between the top quark and the Higgs boson to be less than 2.1 times its expected standard model value at 95% confidence level.

Sirunyan, A. M., et al. (2018). "Search for t(t)over-barH production in the all-jet final state in proton-proton collisions root s=13 TeV." Journal of High Energy Physics(6).
    A search is presented for the associated production of a Higgs boson with a top quark pair in the all-jet final state. Events containing seven or more jets are selected from a sample of proton-proton collisions at root s = 13 TeV collected with the CMS detector at the LHC in 2016, corresponding to an integrated luminosity of 35.9 fb(-1). To separate the t (t) over barH signal from the irreducible t (t) over bar + b (b) over bar background, the analysis assigns leading order matrix element signal and background probability densities to each event. A likelihood-ratio statistic based on these probability densities is used to extract the signal. The results are provided in terms of an observed t (t) over barH signal strength relative to the standard model production cross section mu = sigma/sigma(SM), assuming a Higgs boson mass of 125 GeV. The best fit value is (mu) over cap = 0.9 +/- 0.7(stat) +/- 1.3(syst) = 0.9 +/- 1.5 (tot), and the observed and expected upper limits are, respectively, mu < 3.8 and < 3.1 at 95% confidence levels.

Sirunyan, A. M., et al. (2018). "Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at root s=13 TeV." Journal of High Energy Physics(6).
    A search for flavor-changing neutral currents (FCNC) in events with the top quark and the Higgs boson is presented. The Higgs boson decay to a pair of b quarks is considered. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) recorded by the CMS experiment at the LHC in proton-proton collisions at root s = 13TeV. Two channels are considered: single top quark FCNC production in association with the Higgs boson (pp -> tH), and top quark pair production with FCNC decay of the top quark (t -> qH). Final states with one isolated lepton and at least three reconstructed jets, among which at least two are associated with b quarks, are studied. No significant deviation is observed from the predicted background. Observed (expected) upper limits at 95% confidence level are set on the branching fractions of top quark decays, B(t -> uH) < 0.47% (0.34%) and B(t -> cH) < 0.47% (0.44%), assuming a single nonzero FCNC coupling.

Sirunyan, A. M., et al. (2018). "Search for third-generation scalar leptoquarks decaying to a top quark and a tau lepton at root s=13 TeV." European Physical Journal C 78(9).
    search for pair production of heavy scalar leptoquarks (LQs), each decaying into a top quark and a tau lepton, is presented. The search considers final states with an electron or a muon, one or two tau leptons that decayed to hadrons, and additional jets. The data were collected in 2016 in proton-proton collisions at root s = 13 TeV with the CMS detector at the LHC, and correspond to an integrated luminosity of 35.9fb(-1). No evidence for pair production of LQs is found. Assuming a branching fraction of unity for the decay LQ -> t tau, upper limits on the production cross section are set as a function of LQ mass, excluding masses below 900 GeV at 95% confidence level. These results provide the most stringent limits to date on the production of scalar LQs that decay to a top quark and a tau lepton.

Sirunyan, A. M., et al. (2018). "Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(9).
    A search is presented for resonances decaying to a Z boson and a photon. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1), and collected with the CMS detector at the LHC in 2016. Two decay modes of the Z boson are investigated. In the leptonic channels, the Z boson candidates are reconstructed using electron or muon pairs. In the hadronic channels, they are identified using a large-radius jet, containing either light-quark or b quark decay products of the Z boson, via jet substructure and advanced b quark tagging techniques. The results from these channels are combined and interpreted in terms of upper limits on the product of the production cross section and the branching fraction to Z gamma for narrow and broad spin-0 resonances with masses between 0.35 and 4.0 TeV, providing thereby the most stringent limits on such resonances.

Sirunyan, A. M., et al. (2018). "Search for ZZ resonances in the 2l2v final state in proton-proton collisions at 13 TeV." Journal of High Energy Physics(3).
    A search for heavy resonances decaying to a pair of Z bosons is performed using data collected with the CMS detector at the LHC. Events are selected by requiring two oppositely charged leptons (electrons or muons), consistent with the decay of a Z boson, and large missing transverse momentum, which is interpreted as arising from the decay of a second Z boson to two neutrinos. The analysis uses data from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). The hypothesis of a spin-2 bulk graviton (X) decaying to a pair of Z bosons is examined for 600 4.1 GeV and/or M-Y > 13 GeV, where M-x and M-Y are the masses of the diffractive dissociation systems at negative and positive pseudorapidities, respectively. The results are compared with those from other experiments as well as to predictions from high-energy hadron-hadron interaction models.

Sirunyan, A. M., et al. (2018). "Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer." Journal of High Energy Physics(7).
    The process pp -> pl(+)l(-)p(()*()), with l(+)l(-) a muon or an electron pair produced at midrapidity with mass larger than 110 GeV, has been observed for the first time at the LHC in pp collisions at root s = 13 TeV. One of the two scattered protons is measured in the CMS-TOTEM precision proton spectrometer (CT-PPS), which operated for the first time in 2016. The second proton either remains intact or is excited and then dissociates into a low-mass state p*, which is undetected. The measurement is based on an integrated luminosity of 9.4 fb(-1) collected during standard, high-luminosity LHC operation. A total of 12 mu(+)/mu(-) and 8 e(+)e(-) pairs with m(l(+)l(-)) > 110 GeV, and matching forward proton kinematics, are observed, with expected backgrounds of 1.49 +/- 0.07 (stat) +/- 0.53 (syst) and 2.36 +/- 0.09 (stat) +/- 0.47(syst), respectively. This corresponds to an excess of more than five standard deviations over the expected background. The present result constitutes the first observation of proton-tagged gamma gamma collisions at the electroweak scale. This measurement also demonstrates that CT-PPS performs according to the design specifications.

Sirunyan, A. M., et al. (2018). "Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(10).
    A measurement is presented of the associated production of a single top quark and a W boson in proton -proton collisions at root s = 13 TeV by the CMS Collaboration at the CERN LHC. The data collected corresponds to an integrated luminosity of 35.9 fb(-1). The measurement is performed using events with one electron and one muon in the final state along with at least one jet originated from a bottom quark. A multivariate discriminant, exploiting the kinematic properties of the events, is used to separate the signal from the dominant tt background. The measured cross section of 63.1 +/- 1.8(stat) +/- 6.4(syst) +/- 2.1 (lumi) pb is in agreement with the standard model expectation.

Sirunyan, A. M., et al. (2018). "Precision measurement of the structure of the CMS inner tracking system using nuclear interactions." Journal of Instrumentation 13.
    The structure of the CMS inner tracking system has been studied using nuclear interactions of hadrons striking its material. Data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded in 2015 at the LHC are used to reconstruct millions of secondary vertices from these nuclear interactions. Precise positions of the beam pipe and the inner tracking system elements, such as the pixel detector support tube, and barrel pixel detector inner shield and support rails, are determined using these vertices. These measurements are important for detector simulations, detector upgrades, and to identify any changes in the positions of inactive elements.

Sirunyan, A. M., et al. (2018). "Angular analysis of the decay B+ -> K+mu(+)mu(-) in proton-proton collisions at root s=8 TeV." Physical Review D 98(11).
    The angular distribution of the flavor-changing neutral current decay B+ -> K+mu(+)mu(-) is studied in proton-proton collisions at a center-of-mass energy of 8 TeV. The analysis is based on data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 20.5 fb(-1). The forward-backward asymmetry A(FB) of the dimuon system and the contribution F-H from the pseudoscalar, scalar, and tensor amplitudes to the decay width are measured as a function of the dimuon mass squared. The measurements are consistent with the standard model expectations.

Sirunyan, A. M., et al. (2018). "Elliptic Flow of Charm and Strange Hadrons in High-Multiplicity p plus Pb Collisions at root(NN)-N-s=8.16 TeV." Physical Review Letters 121(8).
    The elliptic azimuthal anisotropy coefficient (upsilon(2)) is measured for charm (D-0) and strange (K-S(0), Lambda, Xi(-), and Omega(-)) hadrons, using a data sample of p + Pb collisions collected by the CMS experiment, at a nucleonnucleon center-of- mass energy of root(NN)-N-s = 8.16 TeV. A significant positive upsilon(2) signal from long- range azimuthal correlations is observed for all particle species in high- multiplicity p + Pb collisions. The measurement represents the first observation of possible long-range collectivity for open heavy flavor hadrons in small systems. The results suggest that charm quarks have a smaller upsilon(2) than the lighter quarks, probably reflecting a weaker collective behavior. This effect is not seen in the larger PbPb collision system at root(NN)-N-s = 5.02 TeV, also presented.

Sirunyan, A. M., et al. (2018). "Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV." European Physical Journal C 78(9).
    Pseudorapidity, transverse momentum, and multiplicity distributions are measured in the pseudorapidity range vertical bar eta vertical bar < 2.4 for charged particles with transverse momenta satisfying pT > 0.5 GeV in proton-proton collisions at a center-of-mass energy of root s = 13 TeV. Measurements are presented in three different event categories. The most inclusive of the categories corresponds to an inelastic pp data set, while the other two categories are exclusive subsets of the inelastic sample that are either enhanced or depleted in single diffractive dissociation events. The measurements are compared to predictions from Monte Carlo event generators used to describe high-energy hadronic interactions in collider and cosmic-ray physics.

Sirunyan, A. M., et al. (2018). "Measurement of jet substructure observables in t(t)over-bar events from proton-proton collisions at root s=13 TeV." Physical Review D 98(9).
    A measurement of jet substructure observables is presented using t (t) over bar events in the lepton + jets channel from proton-proton collisions at root s = 13 TeV recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1). Multiple jet substructure observables are measured for jets identified as bottom, light-quark, and gluon jets, as well as for inclusive jets (no flavor information). The results are unfolded to the particle level and compared to next-to-leading-order predictions from POWHEG interfaced with the parton shower generators PYTHIA 8 and HERWIG 7, as well as from SHERPA 2 and DIRE 2. Avalue of the strong coupling at the Z boson mass, alpha(S)(m(Z)) = 0.115(-0.013)(+0.015), is extracted from the substructure data at leading-order plus leading-log accuracy.

Sirunyan, A. M., et al. (2018). "Measurement of the weak mixing angle using the forward-backward asymmetry of Drell-Yan events in pp collisions at 8 TeV." European Physical Journal C 78(9).
    A measurement is presented of the effective leptonic weak mixing angle (sin(2) theta(effl))using the forward- backward asymmetry of Drell-Yan lepton pairs (mu mu and ee) produced in proton-proton collisions at N root s = 8 TeV at the CMS experiment of the LHC. The data correspond to integrated luminosities of 18.8 and 19.6 fb(-1) in the dimuon and dielectron channels, respectively, containing 8.2 million dimuon and 4.9 million dielectron events. With more events and new analysis techniques, including constraints obtained on the parton distribution functions from the measured forward-backward asymmetry, the statistical and systematic uncertainties are significantly reduced relative to previous CMS measurements. The extracted value of sin(2) theta(effl) from the combined dilepton data is sin(2) theta(effl) = 0.23101 +/- 0.00036 (stat) +/- 0.00018 (syst) 0.00016 (theo) +/- 0.00031 (parton distributions in proton) = 0.23101 +/- 0.00053.

Sirunyan, A. M., et al. (2018). "Observation of the Z -> psi l(+)l(-) Decay in pp Collisions at root s=13 TeV." Physical Review Letters 121(14).
    This Letter presents the observation of the rare Z boson decay Z -> psi l(+)l(-). Here, psi represents contributions from direct J/psi and psi(2S) -> J/psi X, l(+)l(-) is a pair of electrons or muons, and the J/psi meson is detected via its decay to mu(+)mu(-). The sample of proton-proton collision data, collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponds to an integrated luminosity of 35.9 fb(-1). The signal is observed with a significance in excess of 5 standard deviations. After subtraction of the psi(2S) -> J/psi X contribution, the ratio of the branching fraction of the exclusive decay Z -> J/psi X, l(+) l(-) to the decay Z -> mu(+)mu(-)mu(+)mu(-) within a fiducial phase space is measured to be B(Z -> J/psi X, l(+) l(-))/B(Z -> mu(+)mu(-)mu(+)mu(-)) = 0.67 +/- 0.18(stat) +/- 0.05(syst).

Sirunyan, A. M., et al. (2018). "Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at root s=8TeV." Journal of High Energy Physics(11).
    A search for charged Higgs boson decaying to a charm and a bottom quark pair production in which one top quark decays to a charged Higgs boson and a bottom quark and the other decays to a charged lepton, a neutrino, and a bottom quark. Charged Higgs boson decays to are searched for, resulting in a final state containing at least four jets, a charged lepton (muon or electron), and missing transverse momentum. A kinematic fit is performed to identify the pair of jets least likely to be the bottom quarks originating from direct top quark decays and the invariant mass of this pair is used as the final observable in the search. No evidence for the presence of a charged Higgs boson is observed and upper limits at 95% confidence level of 0.8-0.5% are set on the branching fraction B(t H(+)b), assuming B(H+ = 1.0 and B(t H(+)b) + B(t Wb) = 1.0, for the charged Higgs boson mass range 90-150 GeV.

Sirunyan, A. M., et al. (2018). "Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration." Physics Letters B 785: 462-488.
    A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two tau leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton-proton collisions corresponding to an integrated luminosity of 35.9 fb(-1), accumulated by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV. Masses of the pseudoscalar boson between 15 and 60 GeVare probed, and no excess of events above the SM expectation is observed. Upper limits between 3 and 12% are set on the branching fraction B(h -> aa -> 2 tau 2b) assuming the SM production of the Higgs boson. Upper limits are also set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different 2HDM + S scenarios. Assuming the SM production cross section for the Higgs boson, the upper limit on this quantity is as low as 20% for a mass of the pseudoscalar of 40 GeV in the NMSSM. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for beyond the standard model Higgs bosons decaying into a b(b)over-bar pair in pp collisions at root s=13 TeV." Journal of High Energy Physics(8).
    A search for Higgs bosons that decay into a bottom quark-antiquark pair and are accompanied by at least one additional bottom quark is performed with the CMS detector. The data analyzed were recorded in proton-proton collisions at a centre-of-mass energy of root s = 13TeV at the LHC, corresponding to an integrated luminosity of 35.7 fb(-1). The final state considered in this analysis is particularly sensitive to signatures of a Higgs sector beyond the standard model, as predicted in the generic class of two Higgs doublet models (2HDMs). No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons with masses up to 1300 GeV. The results are interpreted within several MSSM and 2HDM scenarios.

Sirunyan, A. M., et al. (2018). "Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(8).
    A search is presented for long-lived charged particles that decay within the CMS detector and produce the signature of a disappearing track. A disappearing track is an isolated track with missing hits in the outer layers of the silicon tracker, little or no energy in associated calorimeter deposits, and no associated hits in the muon detectors. This search uses data collected with the CMS detector in 2015 and 2016 from proton-proton collisions at a center-of-mass energy of 13 TeV at the LHC, corresponding to an integrated luminosity of 38.4 fb(-1). The results of the search are interpreted in the context of the anomaly-mediated supersymmetry breaking model. The data are consistent with the background-only hypothesis. Limits are set on the product of the cross section for direct production of charginos and their branching fraction to a neutralino and a pion, as a function of the chargino mass and lifetime. At 95% confidence level, charginos with masses below 715 (695) GeV are excluded for a lifetime of 3 (7) ns, as are charginos with lifetimes from 0.5 to 60 ns for a mass of 505 GeV. These are the most stringent limits using a disappearing track signature on this signal model for chargino lifetimes above approximate to 0.7 ns.

Sirunyan, A. M., et al. (2018). "Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at root s=13 TeV." Journal of High Energy Physics(11).
    A search for heavy resonances, decaying into the standard model vector bosons and the standard model Higgs boson, is presented. The final states considered contain a b quark-antiquark pair from the decay of the Higgs boson, along with electrons and muons and missing transverse momentum, due to undetected neutrinos, from the decay of the vector bosons. The mass spectra are used to search for a localized excess consistent with a resonant particle. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) collected in 2016 by the CMS experiment at the CERN LHC from proton-proton collisions at a center-of-mass energy of 13 TeV. The data are found to be consistent with background expectations. Exclusion limits are set in the context of spin-0 two Higgs doublet models, some of which include the presence of dark matter. In the spin-1 heavy vector triplet framework, mass-degenerate W and Z resonances with dominant couplings to the standard model gauge bosons are excluded below a mass of 2.9 TeV at 95% confidence level.

Sirunyan, A. M., et al. (2018). "Search for supersymmetry in events with a tau lepton pair and missing transverse momentum in proton-proton collisions at root s=13TeV." Journal of High Energy Physics(11).
    A search for the electroweak production of supersymmetric particles in protonproton collisions at a center-of-mass energy of 13TeV is presented in final states with a tau lepton pair. Both hadronic and leptonic decay modes are considered for the tau leptons. Scenarios involving the direct pair production of tau sleptons, or their indirect production via the decays of charginos and neutralinos, are investigated. The data correspond to an integrated luminosity of 35: 9 fb collected with the CMS detector in 2016. The observed number of events is consistent with the standard model background expectation. The results are interpreted as upper limits on the cross section for tau slepton pair production in di ff erent scenarios. The strongest limits are observed in the scenario of a purely left-handed low mass tau slepton decaying to a nearly massless neutralino. Exclusion limits are also set in the context of simpli fi ed models of chargino-neutralino and chargino pair production with decays to tau leptons, and range up to 710 and 630 GeV, respectively.

Sirunyan, A. M., et al. (2018). "Search for the decay of a Higgs boson in the ll gamma channel in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
    A search for a Higgs boson decaying into a pair of electrons or muons and a photon is described. Higgs boson decays to a Z boson and a photon (H Z , = e or ), or to two photons, one of which has an internal conversion into a muon pair (H (*) ) were considered. The analysis is performed using a data set recorded by the CMS experiment at the LHC from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No significant excess above the background prediction has been found. Limits are set on the cross section for a standard model Higgs boson decaying to opposite-sign electron or muon pairs and a photon. The observed limits on cross section times the corresponding branching fractions vary between 1.4 and 4.0 (6.1 and 11.4) times the standard model cross section for H (*) (H Z ) in the 120-130 GeV mass range of the system. The H (*) and H Z analyses are combined for m(H) =125GeV, obtaining an observed (expected) 95% confidence level upper limit of 3.9 (2.0) times the standard model cross section.

Sirunyan, A. M., et al. (2018). "Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(9).
    A search for the pair production of the lightest supersymmetric partner of the top quark ((t) over tilde (1)) is presented. The search focuses on a compressed scenario where the mass difference between the top squark and the lightest supersymmetric particle, often considered to be the lightest neutralino (( chi) over tilde (0)(1)), is smaller than the mass of the W boson. The proton-proton collision data were recorded by the CMS experiment at a centre-of-mass energy of 13 TeV, and correspond to an integrated luminosity of 35.9 fb(-1). In this search, two decay modes of the top squark are considered: a four-body decay into a bottom quark, two additional fermions, and a (chi) over tilde (1)(0); and a decay via an intermediate chargino. Events are selected using the presence of a high-momentum jet, significant missing transverse momentum, and a low transverse momentum electron or muon. Two analysis techniques are used, targeting different decay modes ((t) over tilde (1)): of the a sequential selection and a multivariate technique. No evidence for the production of top squarks is found, and mass limits at 95% confidence level are set that reach up to 560 GeV, depending on the m((t) over tilde (1)) - m((chi) over tilde (0)(1)) mass difference and the decay mode.

Sirunyan, A. M., et al. (2018). "Search for vector-like T and B quark pairs in final states with leptons at root s=13 TeV." Journal of High Energy Physics(8).
    A search is presented for pair production of heavy vector-like T and B quarks in proton-proton collisions at A root s = 13 TeV. The data sample corresponds to an integrated luminosity of 35.9 fb(-1), collected with the CMS detector at the CERN LHC in 2016. Pair production of T quarks would result in a wide range of final states, since vector-like T quarks of charge 2e/3 are predicted to decay to bW, tZ, and tH. Likewise, vector-like B quarks are predicted to decay to tW, bZ, and bH. Three channels are considered, corresponding to final states with a single lepton, two leptons with the same sign of the electric charge, or at least three leptons. The results exclude T quarks with masses below 1140-1300 GeV and B quarks with masses below 910-1240 GeV for various branching fraction combinations, extending the reach of previous CMS searches by 200-600 GeV.

Sirunyan, A. M., et al. (2018). "Observation of Electroweak Production of Same-Sign W Boson Pairs in the Two Jet and Two Same-Sign Lepton Final State in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 120(8).
    The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-8 effective field theory operators and on the production of doubly charged Higgs bosons.

Sirunyan, A. M., et al. (2018). "Measurements of the pp -> ZZ production cross section and the Z -> 4l branching fraction, and constraints on anomalous triple gauge couplings at root s=13TeV." European Physical Journal C 78(2).
    Four-lepton production in proton-proton collisions, pp -> (Z/gamma*)(Z/gamma*) -> 4l, where l = e or mu, is studied at a center-of-mass energy of 13 TeV with the CMS detector at the LHC. The data sample corresponds to an integrated luminosity of 35.9 fb(-1). The ZZ production cross section, sigma(pp -> ZZ) = 17.2 +/- 0.5 (stat) +/- 0.7 (syst) +/- 0.4 (theo) +/- 0.4 (lumi) pb, measured using events with two opposite-sign, same-flavor lepton pairs produced in the mass region 60 < m(l+l-) < 120 GeV, is consistent with standard model predictions. Differential cross sections are measured and are well described by the theoretical predictions. The Z boson branching fraction to four leptons is measured to be B(Z -> 4l) = 4.83(-0.22)(+0.23) (stat)(-0.29)(+0.32) (syst) +/- 0.08 (theo) +/- 0.12(lumi) x 10(-6) for events with a four-lepton invariant mass in the range 80 < m(4l) < 100 GeV and a dilepton mass m(ll) > 4GeV for all opposite-sign, same-flavor lepton pairs. The results agree with standard model predictions. The invariant mass distribution of the four-lepton system is used to set limits on anomalous ZZZ and ZZ. couplings at 95% confidence level: -0.0012 < f(4)(Z) < 0.0010, -0.0010 < f(5)(Z) < 0.0013, -0.0012 < f(4)(gamma) < 0.0013, -0.0012 < f(5)(gamma) < 0.0013.

Sirunyan, A. M., et al. (2018). "Measurement of associated Z plus charm production in proton-proton collisions at root s=8TeV." European Physical Journal C 78(4).
    A study of the associated production of a Z boson and a charm quark jet (Z + c), and a comparison to production with a b quark jet (Z + b), in pp collisions at a centre-of-mass energy of 8 TeV are presented. The analysis uses a data sample corresponding to an integrated luminosity of 19.7 fb(-1), collected with the CMS detector at the CERN LHC. The Z boson candidates are identified through their decays into pairs of electrons or muons. Jets originating from heavy flavour quarks are identified using semileptonic decays of c or b flavoured hadrons and hadronic decays of charm hadrons. The measurements are performed in the kinematic region with two leptons with pT(l) > 20 GeV, vertical bar eta(l)vertical bar < 2.1, 71 < m(ll) < 111 GeV, and heavy flavour jets with p(T)(jet) > 25 GeV and vertical bar eta(jet)vertical bar < 2.5. The Z + c production cross section is measured to be sigma(pp -> Z + c + X) B(Z -> l(+)l(-)) = 8.8 +/- 0.5 (stat)+/- 0.6 (syst) pb. The ratio of the Z+c and Z+b production cross sections is measured to be sigma(pp -> Z+c+X)/sigma (pp -> Z+b+X) = 2.0 +/- 0.2 (stat)+/- 0.2 (syst). The Z+c production cross section and the cross section ratio are also measured as a function of the transverse momentum of theZ boson and of the heavy flavour jet. The measurements are compared with theoretical predictions.

Sirunyan, A. M., et al. (2018). "Pseudorapidity and transverse momentum dependence of flow harmonics in pPb and PbPb collisions." Physical Review C 98(4).
    Measurements of azimuthal angular correlations are presented for high-multiplicity pPb collisions at root s(NN) = 5.02 TeV and peripheral PbPb collisions at root s(NN) = 2.76 TeV. The data used in this work were collected with the Compact Muon Solenoid (CMS) detector at the European Organization for Nuclear Research (CERN) Large Hadron Collider (LHC). Fourier coefficients as functions of transverse momentum and pseudorapidity are studied using the scalar product method; four-, six-, and eight-particle cumulants; and the Lee-Yang zero technique. The influence of event plane decorrelation is evaluated using the scalar product method and found to account for most of the observed pseudorapidity dependence.

Sirunyan, A. M., et al. (2018). "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at root s=13 TeV." European Physical Journal C 78(7).
    Azimuthal correlations between the two jets with the largest transverse momenta p(T) in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet p(T) up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading p(T) jets are also presented. The analysis is based on data from proton-proton collisions collected by the CMS Collaboration at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). Calculations based on leading-order matrix elements supplemented with parton showering and hadronization do not fully describe the data, so next-to-leading-order calculations matched with parton shower and hadronization models are needed to better describe the measured distributions. Furthermore, we show that azimuthal jet correlations are sensitive to details of the parton showering, hadronization, and multiparton interactions. Anext-to-leading-order calculation matched with parton showers in the MC@NLO method, as implemented in HERWIG 7, gives a better overall description of the measurements than the powheg method.

Sirunyan, A. M., et al. (2018). "Bose-Einstein correlations in pp, pPb, and PbPb collisions at root s(NN)=0.9-7 TeV." Physical Review C 97(6).
    Quantum-statistical (Bose-Einstein) two-particle correlations are measured in pp collisions at root s = 0.9, 2.76, and 7 TeV, as well as in pPb and peripheral PbPb collisions at nucleon-nucleon center-of-mass energies of 5.02 and 2.76 TeV, respectively, using the CMS detector at the Large Hadron Collider. Separate analyses are performed for same-sign unidentified charged particles as well as for same-sign pions and kaons identified via their energy loss in the silicon tracker. The characteristics of the one-, two-, and three-dimensional correlation functions are studied as functions of the pair average transverse momentum (k(T)) and the charged-particle multiplicity in the event. For all systems, the extracted correlation radii steadily increase with the event multiplicity, and decrease with increasing k(T). The radii are in the range 1-5 fm, the largest values corresponding to very high multiplicity pPb interactions and to peripheral PbPb collisions with multiplicities similar to those seen in pPb data. It is also observed that the dependencies of the radii on multiplicity and k(T) largely factorize. At the same multiplicity, the radii are relatively independent of the colliding system and center-of-mass energy.

Sirunyan, A. M., et al. (2018). "Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in pPb and PbPb collisions at the CERN Large Hadron Collider." Physical Review C 97(4).
    Charge-dependent azimuthal correlations of same-and opposite-sign pairs with respect to the second-and third-order event planes have been measured in pPb collisions at root s(NN) = 8.16 TeV and PbPb collisions at 5.02 TeV with the CMS experiment at the LHC. The measurement is motivated by the search for the charge separation phenomenon predicted by the chiral magnetic effect (CME) in heavy ion collisions. Three-and two-particle azimuthal correlators are extracted as functions of the pseudorapidity difference, the transverse momentum (p(T)) difference, and the p(T) average of same-and opposite-charge pairs in various event multiplicity ranges. The data suggest that the charge-dependent three-particle correlators with respect to the second-and third-order event planes share a common origin, predominantly arising from charge-dependent two-particle azimuthal correlations coupled with an anisotropic flow. The CME is expected to lead to a v(2)-independent three-particle correlation when the magnetic field is fixed. Using an event shape engineering technique, upper limits on the v(2)-independent fraction of the three-particle correlator are estimated to be 13% for pPb and 7% for PbPb collisions at 95% confidence level. The results of this analysis, both the dominance of two-particle correlations as a source of the three-particle results and the similarities seen between PbPb and pPb, provide stringent constraints on the origin of charge-dependent three-particle azimuthal correlations and challenge their interpretation as arising from a chiral magnetic effect in heavy ion collisions.

Sirunyan, A. M., et al. (2018). "Constraintson the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at root s=8TeV." Journal of High Energy Physics(2).
    A first search for same-sign WW production via double-parton scattering is performed based on proton-proton collision data at a center-of-mass energy of 8TeV using dimuon and electron-muon final states. The search is based on the analysis of data corresponding to an integrated luminosity of 19.7 fb(-1). No significant excess of events is observed above the expected single-parton scattering yields. A 95% confidence level upper limit of 0.32 pb is set on the inclusive cross section for same-sign WW production via the double-parton scattering process. This upper limit is used to place a 95% confidence level lower limit of 12.2mb on the effective double-parton cross section parameter, closely related to the transverse distribution of partons in the proton. This limit on the effective cross section is consistent with previous measurements as well as with Monte Carlo event generator predictions.

Sirunyan, A. M., et al. (2018). "Inclusive Search for a Highly Boosted Higgs Boson Decaying to a Bottom Quark-Antiquark Pair." Physical Review Letters 120(7).
    An inclusive search for the standard model Higgs boson (H) produced with large transverse momentum (p(T)) and decaying to a bottom quark-antiquark pair (b (b) over bar) is performed using a data set of pp collisions at root s = 13 TeV collected with the CMS experiment at the LHC. The data sample corresponds to an integrated luminosity of 35.9 fb(-1). A highly Lorentz-boosted Higgs boson decaying to b (b) over bar is reconstructed as a single, large radius jet and is identified using jet substructure and dedicated b tagging techniques. The method is validated with Z -> b (b) over bar decays. The Z -> b (b) over bar process is observed for the first time in the single-jet topology with a local significance of 5.1 standard deviations (5.8 expected). For a Higgs boson mass of 125 GeV, an excess of events above the expected background is observed (expected) with a local significance of 1.5 (0.7) standard deviations. The measured cross section times branching fraction for production via gluon fusion of H -> b (b) over bar with p(T) > 450 GeV and in the pseudorapidity range -2.5 K*(0)mu(+)mu(-) are studied using a sample of proton-proton collisions at root s = 8 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 20.5 fb(-1). An angular analysis is performed to determine the P-1 and P-5' parameters, where the P-5' parameter is of particular interest because of recent measurements that indicate a potential discrepancy with the standard model predictions. Based on a sample of 1397 signal events, the P-1 and P-5' parameters are determined as a function of the dimuon invariant mass squared. The measurements are in agreement with predictions based on the standard model. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Measurement of b hadron lifetimes in pp collisions at root s = 8TeV (vol 78, 2018)." European Physical Journal C 78(7).
    
Sirunyan, A. M., et al. (2018). "Measurement of differential cross sections in the kinematic angular variable phi* for inclusive Z boson production in pp collisions at root s=8 TeV." Journal of High Energy Physics(3).
    Measurements of differential cross sections d sigma/d phi* and double-differential cross sections d(2)sigma/ld phi*d/y/ for inclusive Z boson production are presented using the dielectron and dimuon final states. The kinematic observable phi* correlates with the dilepton transverse momentum but has better resolution, and y is the dilepton rapidity. The analysis is based on data collected with the CMS experiment at a centre-of-mass energy of 8 TeV corresponding to an integrated luminosity of 19.7 fb(-1). The normalised cross section (1/sigma) d sigma/d phi*, within the fiducial kinematic region, is measured with a precision of better than 0.5% for phi* < 1. The measurements are compared to theoretical predictions and they agree, typically, within few percent.

Sirunyan, A. M., et al. (2018). "Measurement of normalized differential t(t)over-bar cross sections in the dilepton channel from pp collisions at root s=13 TeV." Journal of High Energy Physics(4).
    Normalized differential cross sections for top quark pair production are measured in the dilepton (e(+)e(-), mu(+)mu(-), and mu(-/+),e(+/-)) decay channels in proton-proton collisions at a center-of-mass energy of 13 TeV. The measurements are performed with data corresponding to an integrated luminosity of 2.1 fb(-1) using the CMS detector at the LHC. The cross sections are measured differentially as a function of the kinematic properties of the leptons, jets from bottom quark hadronization, top quarks, and top quark pairs at the particle and parton levels. The results are compared to several Monte Carlo generators that implement calculations up to next-to-leading order in perturbative quantum chromodynamics interfaced with parton showering, and also to fixed-order theoretical calculations of top quark pair production up to next-to-next-to-leading order.

Sirunyan, A. M., et al. (2018). "Measurement of prompt and nonprompt charmonium suppression in PbPb collisions at 5.02 TeV." European Physical Journal C 78(6).
    The nuclear modification factors of J/psi and psi(2S) mesons are measured in PbPb collisions at a centre-of-mass energy per nucleon pair of root S-NN = 5.02 TeV. The analysis is based on PbPb and pp data samples collected by CMS at the LHC in 2015, corresponding to integrated luminosities of 464 mu b(-1) and 28 pb(-1), respectively. The measurements are performed in the dimuon rapidity range of vertical bar y vertical bar < 2.4 as a function of centrality, rapidity, and transverse momentum (p(T)) from p(T) = 3 GeV/c in the most forward region and up to 50 GeV/c. Both prompt and nonprompt (coming from b hadron decays) J/psi mesons are observed to be increasingly suppressed with centrality, with a magnitude similar to the one observed at root S-NN = 2.76 TeV for the two J/psi meson components. No dependence on rapidity is observed for either prompt or nonprompt J/psi mesons. An indication of a lower prompt J/psi meson suppression at p(T) > 25 GeV/c is seen with respect to that observed at intermediate p(T). The prompt psi(2S) meson yield is found to be more suppressed than that of the prompt J/psi mesons in the entire p(T) range.

Sirunyan, A. M., et al. (2018). "Measurement of Prompt D-0 Meson Azimuthal Anisotropy in Pb-Pb Collisions at root S-NN=5.02 TeV." Physical Review Letters 120(20).
    The prompt D-0 meson azimuthal anisotropy coefficients, v(2) and ?v(3), are measured at midrapidity ( |y| < 1.0) in Pb-Pb collisions at a center-of-mass energy root s(NN) = 5.02 TeV per nucleon pair with data collected by the CMS experiment. The measurement is performed in the transverse momentum (p(T)) range of 1 to 40 GeV/c, for central and midcentral collisions. The v(2) coefficient is found to be positive throughout the p(T) range studied. The first measurement of the prompt D-0 meson v(3) coefficient is performed, and values up to 0.07 are observed for p(T) around 4 GeV/c. Compared to measurements of charged particles, a similar p(T) dependence, but smaller magnitude for p(T) < 6 GeV/r, is found for prompt D-0 meson v(2) and v(3) coefficients. The results are consistent with the presence of collective motion of charm quarks at low p(r) and a path length dependence of charm quark energy loss at high p(r), thereby providing new constraints on the theoretical description of the interactions between charm quarks and the quark-gluon plasma.

Sirunyan, A. M., et al. (2018). "Measurement of quarkonium production cross sections in pp collisions at root s=13 TeV." Physics Letters B 780: 251-272.
    Differential production cross sections of prompt J/psi and psi(2S) charmonium and Upsilon(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at root s = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb(-1) for the J/psi and 2.7 fb(-1) for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity vertical bar y vertical bar < 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Upsilon(2S) to Upsilon(1S), and Upsilon(3S) to Upsilon(1S) production. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Measurement of the Splitting Function in &ITpp &ITand Pb-Pb Collisions at root&ITsNN&IT=5.02 TeV." Physical Review Letters 120(14).
    Data from heavy ion collisions suggest that the evolution of a parton shower is modified by interactions with the color charges in the dense partonic medium created in these collisions, but it is not known where in the shower evolution the modifications occur. The momentum ratio of the two leading partons, resolved as subjets, provides information about the parton shower evolution. This substructure observable, known as the splitting function, reflects the process of a parton splitting into two other partons and has been measured for jets with transverse momentum between 140 and 500 GeV, in pp and PbPb collisions at a center-of-mass energy of 5.02 TeV per nucleon pair. In central PbPb collisions, the splitting function indicates a more unbalanced momentum ratio, compared to peripheral PbPb and pp collisions.. The measurements are compared to various predictions from event generators and analytical calculations.

Sirunyan, A. M., et al. (2018). "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(7).
    This paper presents a measurement of the underlying event activity in proton-proton collisions at a center-of-mass energy of 13TeV, performed using inclusive Z boson production events collected with the CMS experiment at the LHC. The analyzed data correspond to an integrated luminosity of 2.1 fb(-1). The underlying event activity is quantified in terms of the charged particle multiplicity, as well as of the scalar sum of the charged particles' transverse momenta in different topological regions defined with respect to the Z boson direction. The distributions are unfolded to the stable particle level and compared with predictions from various Monte Carlo event generators, as well as with similar CDF and CMS measurements at center-of-mass energies of 1.96 and 7TeV respectively.

Sirunyan, A. M., et al. (2018). "Measurements of the pp -> ZZ production cross section and the Z -> 4l branching fraction, and constraints on anomalous triple gauge couplings at root s = 13 TeV (vol 78, 165, 2018)." European Physical Journal C 78(6).
    
Sirunyan, A. M., et al. (2018). "Nuclear modification factor of D-0 mesons in PbPb collisions at root s(NN)=5.02 TeV." Physics Letters B 782: 474-496.
    The transverse momentum (p(T)) spectrum of prompt D-0 mesons and their antiparticles has been measured via the hadronic decay channels D-0 -> K- pi(+) and (D) over bar (0) -> K+ pi(-) in pp and PbPb collisions at a centre-of-mass energy of 5.02 TeV per nucleon pair with the CMS detector at the LHC. The measurement is performed in the D-0 meson p(T) range of 2-100GeV/c and in the rapidity range of vertical bar y vertical bar < 1. The pp (PbPb) dataset used for this analysis corresponds to an integrated luminosity of 27.4 pb(-1) (530 mu b(-1)). The measured D-0 meson p(T) spectrum in pp collisions is well described by perturbative QCD calculations. The nuclear modification factor, comparing D-0 meson yields in PbPb and pp collisions, was extracted for both minimum-bias and the 10% most central PbPb interactions. For central events, the D-0 meson yield in the PbPb collisions is suppressed by a factor of 5-6 compared to the pp reference in the p(T) range of 6-10GeV/c. For D-0 mesons in the high-p(T) range of 60-100GeV/c, a significantly smaller suppression is observed. The results are also compared to theoretical calculations. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Observation of Correlated Azimuthal Anisotropy Fourier Harmonics in pp and p plus Pb Collisions at the LHC." Physical Review Letters 120(9).
    The azimuthal anisotropy Fourier coefficients (v(n)) in 8.16 TeV p + Pb data are extracted via long-range two-particle correlations as a function of the event multiplicity and compared to corresponding results in pp and PbPb collisions. Using a four-particle cumulant technique, v(n) correlations are measured for the first time in pp and p + Pb collisions. The v(2) and v(4) coefficients are found to be positively correlated in all collision systems. For high-multiplicity p + Pb collisions, an anticorrelation of v(2) and v(3) is observed, with a similar correlation strength as in PbPb data at the same multiplicity. The new correlation results strengthen the case for a common origin of the collectivity seen in p + Pb and PbPb collisions in the measured multiplicity range.

Sirunyan, A. M., et al. (2018). "Observation of the Higgs boson decay to a pair of tau leptons with the CMS detector." Physics Letters B 779: 283-316.
    A measurement of the H -> tau tau signal strength is performed using events recorded in proton-proton collisions by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13TeV. The data set corresponds to an integrated luminosity of 35.9 fb(-1). The H -> tau tau signal is established with a significance of 4.9 standard deviations, to be compared to an expected significance of 4.7 standard deviations. The best fit of the product of the observed H -> tau tau signal production cross section and branching fraction is 1.09(-0.2)(6+0.27) times the standard model expectation. The combination with the corresponding measurement performed with data collected by the CMS experiment at center-of-mass energies of 7 and 8 TeV leads to an observed significance of 5.9 standard deviations, equal to the expected significance. This is the first observation of Higgs boson decays to tau leptons by a single experiment. (c) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for a massive resonance decaying to a pair of Higgs bosons in the four b quark final state in proton-proton collisions at root s=13 TeV." Physics Letters B 781: 244-269.
    A search for a massive resonance decaying into a pair of standard model Higgs bosons, in a final state consisting of two b quark-antiquark pairs, is performed. A data sample of proton-proton collisions at a centre-of-mass energy of 13 TeV is used, collected by the CMS experiment at the CERN LHC in 2016, and corresponding to an integrated luminosity of 35.9 fb(-1). The Higgs bosons are highly Lorentz-boosted and are each reconstructed as a single large-area jet. The signal is characterized by a peak in the dijet invariant mass distribution, above a background from the standard model multijet production. The observations are consistent with the background expectations, and are interpreted as upper limits on the products of the s-channel production cross sections and branching fractions of narrow bulk gravitons and radions in warped extra-dimensional models. The limits range from 126 to 1.4 fb at 95% confidence level for resonances with masses between 750 and 3000 GeV, and are the most stringent to date, over the explored mass range. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at root s=13 TeV." Journal of High Energy Physics(6).
    A search for dark matter is conducted in events with large missing transverse momentum and a hadronically decaying, Lorentz-boosted top quark. This study is performed using proton-proton collisions at a center-of-mass energy of 13 TeV, in data recorded by the CMS detector in 2016 at the LHC, corresponding to an integrated luminosity of 36 fb(-1). New substructure techniques, including the novel use of energy correlation functions, are utilized to identify the decay products of the top quark. With no significant deviations observed from predictions of the standard model, limits are placed on the production of new heavy bosons coupling to dark matter particles. For a scenario with purely vector-like or purely axial-vector-like flavor changing neutral currents, mediator masses between 0.20 and 1.75 TeV are excluded at 95% confidence level, given a sufficiently small dark matter mass. Scalar resonances decaying into a top quark and a dark matter fermion are excluded for masses below 3.4 TeV, assuming a dark matter mass of 100 GeV.

Sirunyan, A. M., et al. (2018). "Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
    Results are presented from a search for the direct electroweak production of charginos and neutralinos in signatures with either two or more leptons (electrons or muons) of the same electric charge, or with three or more leptons, which can include up to two hadronically decaying tau leptons. The results are based on a sample of proton proton collision data collected at root s = 13 TeV, recorded with the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1). The observed event yields are consistent with the expectations based on the standard model. The results are interpreted in simplified models of supersymmetry describing various scenarios for the production and decay of charginos and neutralinos. Depending on the model parameters chosen, mass values between 180 GeV and 1150 GeV are excluded at 95% CL. These results significantly extend the parameter space probed for these particles in searches at the LHC. In addition, results are presented in a form suitable for alternative theoretical interpretations.

Sirunyan, A. M., et al. (2018). "Search for excited quarks of light and heavy flavor in gamma plus jet final states in proton-proton collisions at root s=13 TeV." Physics Letters B 781: 390-411.
    A search is presented for excited quarks of light and heavy flavor that decay to gamma + jet final states. The analysis is based on data corresponding to an integrated luminosity of 35.9 fb(-1) collected by the CMS experiment in proton-proton collisions at root s = 13 TeV at the LHC. A signal would appear as a resonant contribution to the invariant mass spectrum of the gamma + jet system, above the background expected from standard model processes. No resonant excess is found, and upper limits are set on the product of the excited quark cross section and its branching fraction as a function of its mass. These are the most stringent limits to date in the gamma + jet final state, and exclude excited light quarks with masses below 5.5 TeV and excited b quarks with masses below 1.8 TeV, assuming standard model like coupling strengths. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for gauge-mediated supersymmetry in events with at least one photon and missing transverse momentum in pp collisions at ,root s=13 TeV." Physics Letters B 780: 118-143.
    A search for gauge-mediated supersymmetry (SUSY) in final states with photons and large missing transverse momentum is presented. The data sample of pp collisions at root s= 13 TeV was collected with the CMS detector at the CERN LHC and corresponds to an integrated luminosity of 35.9 fb(-1). Data are compared with models in which the lightest neutralino has bino- or wino-like components, resulting in decays to photons and gravitinos, where the gravitinos escape detection. The event selection is optimized for both electroweak (EWK) and strong production SUSY scenarios. The observed data are consistent with standard model predictions, and limits are set in the context of a general gauge mediation model in which gaugino masses up to 980 GeV are excluded at 95% confidence level. Gaugino masses below 780 and 950 GeV are excluded in two simplified models with EWK production of mass-degenerate charginos and neutralinos. Stringent limits are set on simplified models based on gluino and squark pair production, excluding gluino (squark) masses up to 2100 (1750)GeV depending on the assumptions made for the decay modes and intermediate particle masses. This analysis sets the highest mass limits to date in the studied EWK models, and in the considered strong production models when the mass difference between the gauginos and the squarks or gluinos is small. (C) 2018 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for heavy resonances decaying to a top quark and a bottom quark in the lepton plus jets final state in proton-proton collisions at 13 TeV." Physics Letters B 777: 39-63.
    A search is presented for narrow heavy resonances decaying to a top quark and a bottom quark using data collected by the CMS experiment at root s= 13 TeV in 2016. The data set analyzed corresponds to an integrated luminosity of 35.9fb(-1). Final states that include a single lepton (e, mu), multiple jets, and missing transverse momentum are analyzed. No evidence is found for the production of a W' boson, and the production of right-handed W' bosons is excluded at 95% confidence level for masses up to 3.6 TeV depending on the scenario considered. Exclusion limits for W' bosons are also presented as a function of their coupling strength to left- and right-handed fermions. These limits on a W' boson decaying via a top and a bottom quark are the most stringent published to date. (c) 2017 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton-proton collisions at root s=13 TeV." Physics Letters B 778: 101-127.
    A search for the production of Higgs boson pairs in proton-proton collisions at a centre-of-mass energy of 13TeVis presented, using a data sample corresponding to an integrated luminosity of 35.9fb(-1) collected with the CMS detector at the LHC. Events with one Higgs boson decaying into two bottom quarks and the other decaying into two tau leptons are explored to investigate both resonant and nonresonant production mechanisms. The data are found to be consistent, within uncertainties, with the standard model background predictions. For resonant production, upper limits at the 95% confidence level are set on the production cross section for Higgs boson pairs as a function of the hypothesized resonance mass and are interpreted in the context of the minimal supersymmetric standard model. For nonresonant production, upper limits on the production cross section constrain the parameter space for anomalous Higgs boson couplings. The observed (expected) upper limit at 95% confidence level corresponds to about 30(25) times the prediction of the standard model. (C) 2018 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for Higgsino pair production in pp collisions at root s=13 TeV in final states with large missing transverse momentum and two Higgs bosons decaying via H -> b(b)over bar." Physical Review D 97(3).
    Results are reported from a search for new physics in 13 TeV proton-proton collisions in the final state with large missing transverse momentum and two Higgs bosons decaying via H -> b(b)over bar. The search uses a data sample accumulated by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of 35.9 fb(-1). The search is motivated by models based on gauge-mediated supersymmetry breaking, which predict the electroweak production of a pair of Higgsinos, each of which can decay via a cascade process to a Higgs boson and an undetected lightest supersymmetric particle. The observed event yields in the signal regions are consistent with the standard model background expectation obtained from control regions in data. Higgsinos in the mass range 230-770 GeV are excluded at 95% confidence level in the context of a simplified model for the production and decay of approximately degenerate Higgsinos.

Sirunyan, A. M., et al. (2018). "Search for lepton flavour violating decays of the Higgs boson to mu tau and e tau in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(6).
    A search for lepton flavour violating decays of the Higgs boson in the mu tau and e tau decay modes is presented. The search is based on a data set corresponding to an integrated luminosity of 35.9 fb(-1) of proton-proton collisions collected with the CMS detector in 2016, at a centre-of-mass energy of 13 TeV. No significant excess over the standard model expectation is observed. The observed (expected) upper limits on the lepton flavour violating branching fractions of the Higgs boson are B(H -> mu tau) < 0.25% (0.25%) and B(H -> e tau) < 0.61% (0.37%), at 95% confidence level. These results are used to derive upper limits on the off-diagonal mu tau and e tau Yukawa couplings root vertical bar Y-mu tau vertical bar(2) + vertical bar Y-mu tau vertical bar(2) < 1.43 x 10(-3) and root vertical bar Y-e tau vertical bar(2) + vertical bar Y-tau e vertical bar(2) < 2.26 x 10(-3) at 95% confidence level. The limits on the lepton flavour violating branching fractions of the Higgs boson and on the associated Yukawa couplings are the most stringent to date.

Sirunyan, A. M., et al. (2018). "Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(1).
    A search for narrow vector resonances decaying into quark-antiquark pairs is presented. The analysis is based on data collected in proton-proton collisions at root s = 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1). The hypothetical resonance is produced with sufficiently high transverse momentum that its decay products are merged into a single jet with two-prong substructure. A signal would be identified as a peak over a smoothly falling background in the distribution of the invariant mass of the jet, using novel jet substructure techniques. No evidence for such a resonance is observed within the mass range of 50-300 GeV. Upper limits at 95% confidence level are set on the production cross section, and presented in a mass-coupling parameter space. The limits further constrain simplified models of dark matter production involving a mediator interacting between quarks and dark matter particles through a vector or axial-vector current. In the framework of these models, the results are the most sensitive to date, extending for the first time the search region to masses below 100 GeV.

Sirunyan, A. M., et al. (2018). "Search for massive resonances decaying into WW, WZ, ZZ, qW, and qZ with dijet final states at root s=13 TeV." Physical Review D 97(7).
    Results are presented from a search in the dijet final state for new massive narrow resonances decaying to pairs of W and Z bosons or to a W/Z boson and a quark. Results are based on data recorded in proton-proton collisions at root s = 13 TeV with the CMS detector at the CERN LHC. The data correspond to an integrated luminosity of 35.9 fb(-1). The mass range investigated extends upwards from 1.2 TeV. No excess is observed above the estimated standard model background and limits are set at 95% confidence level on cross sections, which are interpreted in terms of various models that predict gravitons, heavy spin-1 bosons, and excited quarks. In a heavy vector triplet model, W' and Z' resonances, with masses below 3.2 and 2.7 TeV, respectively, and spin-1 resonances with degenerate masses below 3.8 TeV are excluded at 95% confidence level. In the case of a singlet W' resonance masses between 3.3 and 3.6 TeV can be excluded additionally. Similarly, excited quark resonances, q*, decaying to qW and qZ with masses less than 5.0 and 4.7 TeV, respectively, are excluded. In a narrow-width bulk graviton model, upper limits are set on cross sections ranging from 0.6 fb for high resonance masses above 3.6 TeV, to 36.0 fb for low resonance masses of 1.3 TeV.

Sirunyan, A. M., et al. (2018). "Search for new long-lived particles at root s=13 TeV." Physics Letters B 780: 432-454.
    A search for long-lived particles was performed with data corresponding to an integrated luminosity of 2.6 fb(-1) collected at a center-of-mass energy of 13 TeV by the CMS experiment in 2015. The analysis exploits two customized topological trigger algorithms, and uses the multiplicity of displaced jets to search for the presence of a signal decay occurring at distances between 1 and 1000 mm. The results can be interpreted in a variety of different models. For pair-produced long-lived particles decaying to two b quarks and two leptons with equal decay rates between lepton flavors, cross sections larger than 2.5 fb are excluded for proper decay lengths between 70-100 mm for a long-lived particle mass of 1130 GeV at 95% confidence. For a specific model of pair-produced, long-lived top squarks with R-parity violating decays to a b quark and a lepton, masses below 550-1130 GeV are excluded at 95% confidence for equal branching fractions between lepton flavors, depending on the squark decay length. This mass bound is the most stringent to date for top squark proper decay lengths greater than 3 mm. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at root s=13TeV." Journal of High Energy Physics(3).
    Search results are presented for physics beyond the standard model in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) of proton-proton collisions at root s = 13TeV collected with the CMS detector at the LHC in 2016. The analysis uses the invariant mass of the lepton pair, searching for a kinematic edge or a resonant-like excess compatible with the Z boson mass. The search for a kinematic edge targets production of particles sensitive to the strong force, while the resonance search targets both strongly and electroweakly produced new physics. The observed yields are consistent with the expectations from the standard model, and the results are interpreted in the context of simplified models of supersymmetry. In a gauge mediated supersymmetry breaking (GMSB) model of gluino pair production with decay chains including Z bosons, gluino masses up to 1500-1770 GeV are excluded at the 95% confidence level depending on the lightest neutralino mass. In a model of electroweak chargino-neutralino production, chargino masses as high as 610 GeV are excluded when the lightest neutralino is massless. In GMSB models of electroweak neutralino-neutralino production, neutralino masses up to 500-650 GeV are excluded depending on the decay mode assumed. Finally, in a model with bottom squark pair production and decay chains resulting in a kinematic edge in the dilepton invariant mass distribution, bottom squark masses up to 980-1200 GeV are excluded depending on the mass of the next-to-lightest neutralino.

Sirunyan, A. M., et al. (2018). "Search for pair production of vector-like quarks in the bW(b)over-barW channel from proton-proton collisions at root s=13TeV." Physics Letters B 779: 82-106.
    A search is presented for the production of vector-like quark pairs, T (T) over bar or Y (Y) over bar, with electric charge of 2/3(T) or -4/3(Y), in proton-proton collisions at root s= 13 TeV. The data were collected by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.8 fb(-1). The T and Y quarks are assumed to decay exclusively to a W boson and a b quark. The search is based on events with a single isolated electron or muon, large missing transverse momentum, and at least four jets with large transverse momenta. In the search, a kinematic reconstruction of the final state observables is performed, which would permit a signal to be detected as a narrow mass peak (approximate to 7% resolution). The observed number of events is consistent with the standard model prediction. Assuming strong pair production of the vector-like quarks and a 100% branching fraction to bW, a lower limit of 1295 GeV at 95% confidence level is set on the T and Y quark masses. (c) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for resonant and nonresonant Higgs boson pair production in the b(b)over-barl nu l nu final state in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(1).
    Searches for resonant and nonresonant pair-produced Higgs bosons (HH) decaying respectively into l nu l nu, through either W or Z bosons, and b (b) over bar are presented. The analyses are based on a sample of proton-proton collisions at root s = 13 TeV, collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1). Data and predictions from the standard model are in agreement within uncertainties. For the standard model HH hypothesis, the data exclude at 95% confidence level a product of the production cross section and branching fraction larger than 72 fb, corresponding to 79 times the standard model prediction. Constraints are placed on different scenarios considering anomalous couplings, which could affect the rate and kinematics of HH production. Upper limits at 95% confidence level are set on the production cross section of narrow-width spin-0 and spin-2 particles decaying to Higgs boson pairs, the latter produced with minimal gravity-like coupling.

Sirunyan, A. M., et al. (2018). "Search for single production of a vector- like T quark decaying to a Z boson and a top quark in proton-proton collisions at root s=13 TeV." Physics Letters B 781: 574-600.
    A search is presented for single production of a vector-like quark (T) decaying to a Z boson and a top quark, with the Z boson decaying leptonically and the top quark decaying hadronically. The search uses data collected by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV in 2016, corresponding to an integrated luminosity of 35.9 fb(-1). The presence of forward jets is a particular characteristic of single production of vector-like quarks that is used in the analysis. For the first time, different T quark width hypotheses are studied, from negligibly small to 30% of the new particle mass. At the 95% confidence level, the product of cross section and branching fraction is excluded above values in the range 0.26-0.04 pb for T quark masses in the range 0.7-1.7 TeV, assuming a negligible width. A similar sensitivity is observed for widths of up to 30% of the T quark mass. The production of a heavy Z' boson decaying to Tt, with T -> tZ, is also searched for, and limits on the product of cross section and branching fractions for this process are set between 0.13 and 0.06pbfor Z' boson masses in the range from 1.5 to 2.5 TeV. (C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(2).
    A search for new physics is carried out in events with at least three electrons or muons in any combination, jets, and missing transverse momentum. Results are based on the sample of proton-proton collision data produced by the LHC at a center-of-mass energy of 13TeV and collected by the CMS experiment in 2016. The data sample analyzed corresponds to an integrated luminosity of 35.9 fb(-1). Events are classified according to the number of b jets, missing transverse momentum, hadronic transverse momentum, and the invariant mass of same-flavor dilepton pairs with opposite charge. No significant excess above the expected standard model background is observed. Exclusion limits at 95% confidence level are computed for four different supersymmetric simplified models with pair production of gluinos or third-generation squarks. In the model with gluino pair production, with subsequent decays into a top quark-antiquark pair and a neutralino, gluinos with masses smaller than 1610 GeV are excluded for a massless lightest supersymmetric particle. In the case of bottom squark pair production, the bottom squark masses are excluded up to 840 GeV for charginos lighter than 200 GeV. For a simplified model of heavy top squark pair production, the (t) over tilde (2) mass is excluded up to 720, 780, or 710 GeV for models with an exclusive (t) over tilde (2) -> (t) over tilde H-1 decay, an exclusive (t) over tilde (2) -> (t) over tilde (1)Z decay, or an equally probable mix of those two decays. In order to provide a simplified version of the analysis for easier interpretation, a small set of aggregate signal regions also has been de fined, providing a compromise between simplicity and analysis sensitivity.

Sirunyan, A. M., et al. (2018). "Search for supersymmetry in events with one lepton and multiple jets exploiting the angular correlation between the lepton and the missing transverse momentum in proton-proton collisions at root s=13 TeV." Physics Letters B 780: 384-409.
    Results are presented from a search for supersymmetry in events with a single electron or muon and hadronic jets. The data correspond to a sample of proton-proton collisions at root s = 13 TeV with an integrated luminosity of 35.9 fb(-1), recorded in 2016 by the CMS experiment. A number of exclusive search regions are defined according to the number of jets, the number of b-tagged jets, the scalar sum of the transverse momenta of the jets, and the scalar sum of the missing transverse momentum and the transverse momentum of the lepton. Standard model background events are reduced significantly by requiring a large azimuthal angle between the direction of the lepton and of the reconstructed W boson, computed under the hypothesis that all of the missing transverse momentum in the event arises from a neutrino produced in the leptonic decay of the W boson. The numbers of observed events are consistent with the expectations from standard model processes, and the results are used to set lower limits on supersymmetric particle masses in the context of two simplified models of gluino pair production. In the first model, where each gluino decays to a top quark-antiquark pair and a neutralino, gluino masses up to 1.8 TeV are excluded at the 95% CL. The second model considers a three-body decay to a light quark-antiquark pair and a chargino, which subsequently decays to a W boson and a neutralino. In this model, gluinos are excluded up to 1.9 TeV. (C) 2018 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at root s=13 TeV." Physics Letters B 779: 166-190.
    An inclusive search for anomalous Higgs boson production in the diphoton decay channel and in association with at least one jet is presented, using LHC proton-proton collision data collected by the CMS experiment at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 35.9 fb(-1). The razor variables M-R and R-2, as well as the momentum and mass resolution of the diphoton system, are used to categorize events into different search regions. The search result is interpreted in the context of strong and electroweak production of supersymmetric particles. We exclude bottom squark pair-production with masses below 450 GeV for bottom squarks decaying to a bottom quark, a Higgs boson, and the lightest supersymmetric particle (LSP) for LSP masses below 250 GeV. For wino-like chargino-neutralino production, we exclude charginos with mass below 170 GeV for LSP masses below 25 GeV. In the GMSB scenario, we exclude charginos with mass below 205 GeV for neutralinos decaying to a Higgs boson and a goldstino LSP with 100% branching fraction. C) 2018 The Author(s). Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for the pair production of third-generation squarks with two-body decays to a bottom or charm quark and a neutralino in proton-proton collisions at root s=13 TeV." Physics Letters B 778: 263-291.
    Results are presented from a search for the pair production of third-generation squarks in proton-proton collision events with two-body decays to bottom or charm quarks and a neutralino, which produces a significant imbalance in the transverse momentum. The search is performed using a sample of proton-proton collision data at root s = 13 TeV recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9fb(-1). No statistically significant excess of events is observed beyond the expected contribution from standard model processes. Exclusion limits are set in the context of simplified models of bottom or top squark pair production. Models with bottom squark masses up to 1220 GeV are excluded at 95% confidence level for light neutralinos, and models with top squark masses of 510 GeV are excluded assuming that the mass splitting between the top squark and the neutralino is small. (C) 2018 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Study of jet quenching with isolated-photon plus jet correlations in PbPb and pp collisions at root s(NN)=5.02 TeV." Physics Letters B 785: 14-39.
    Measurements of azimuthal angle and transverse momentum (p(T)) correlations of isolated photons and associated jets are reported for pp and PbPb collisions at root s(NN) = 5.02 TeV. The data were recorded with the CMS detector at the CERN LHC. For events containing a leading isolated photon with p(T)(gamma) > 40 GeV/c and an associated jet with p(T)(jet) > 30 GeV/c, the photon+jet azimuthal correlation and p(T) imbalance in PbPb collisions are studied as functions of collision centrality and p(T)(gamma). The results are compared to pp reference data collected at the same collision energy and to predictions from several theoretical models for parton energy loss. No evidence of broadening of the photon+jet azimuthal correlations is observed, while the ratio p(T)(jet)/p(T)(gamma) decreases significantly for PbPb data relative to the pp reference. All models considered agree within uncertainties with the data. The number of associated jets per photon with p(T)(gamma) > 80GeV/c is observed to be shifted towards lower p(T)(jet) in central PbPb collisions compared to pp collisions. (C) 2018 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(3).
    A statistical combination of several searches for the electroweak production of charginos and neutralinos is presented. All searches use proton-proton collision data at A root s = 13 TeV, recorded with the CMS detector at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb(-1). In addition to the combination of previous searches, a targeted analysis requiring three or more charged leptons (electrons or muons) is presented, focusing on the challenging scenario in which the difference in mass between the two least massive neutralinos is approximately equal to the mass of the Z boson. The results are interpreted in simplified models of chargino-neutralino or neutralino pair production. For chargino-neutralino production, in the case when the lightest neutralino is massless, the combination yields an observed (expected) limit at the 95% confidence level on the chargino mass of up to 650 (570) GeV, improving upon the individual analysis limits by up to 40 GeV. If the mass difference between the two least massive neutralinos is approximately equal to the mass of the Z boson in the chargino-neutralino model, the targeted search requiring three or more leptons obtains observed and expected exclusion limits of around 225 GeV on the second neutralino mass and 125 GeV on the lightest neutralino mass, improving the observed limit by about 60 GeV in both masses compared to the previous CMS result. In the neutralino pair production model, the combined observed (expected) exclusion limit on the neutralino mass extends up to 650-750 (550-750) GeV, depending on the branching fraction assumed. This extends the observed exclusion achieved in the individual analyses by up to 200 GeV. The combined result additionally excludes some intermediate gaps in the mass coverage of the individual analyses.

Sirunyan, A. M., et al. (2018). "Measurement of the inclusive t(t)over-bar cross section in pp collisions root s=5.02 TeV using final states with at least one charged lepton." Journal of High Energy Physics(3).
    The top quark pair production cross section (ad) is measured for the first time in pp collisions at a center-of-mass energy of 5.02 TeV. The data were collected by the CMS experiment at the LHC and correspond to an integrated luminosity of 27.4 pb(-1). The measurement is performed by analyzing events with at least one charged lepton. The measured cross section is sigma(tt) = 69.5 +/- 6.1 (stat) +/- 5.6 (syst) +/- 1.6 (lumi) pb, with a total relative uncertainty of 12%. The result is in agreement with the expectation from the standard model. The impact of the presented measurement on the determination of the gluon distribution function is investigated.

Sirunyan, A. M., et al. (2018). "Search for top squarks and dark matter particles in opposite-charge dilepton final states at root s=13 TeV." Physical Review D 97(3).
    A search for new physics is presented in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum (p(T)(miss)). The search uses proton-proton collision data at root s = 13 TeV amounting to 35.9 fb(-1) of integrated luminosity collected using the CMS detector in 2016. Hypothetical signal events are efficiently separated from the dominant t (t) over bar background with requirements on p(T)(miss) and transverse-mass variables. No significant deviation is observed from the expected background. Exclusion limits are set in the context of simplified supersymmetric models with pair-produced top squarks. For top squarks, decaying exclusively to a top quark and a neutralino, exclusion limits are placed at 95% confidence level on the mass of the lightest top squark up to 800 GeVand on the lightest neutralino up to 360 GeV. These results, combined with searches in the single-lepton and all-jet final states, raise the exclusion limits up to 1050 GeV for the lightest top squark and up to 500 GeV for the lightest neutralino. For top squarks undergoing a cascade decay through charginos and sleptons, the mass limits reach up to 1300 GeV for top squarks and up to 800 GeV for the lightest neutralino. The results are also interpreted in a simplified model with a dark matter (DM) particle coupled to the top quark through a scalar or pseudoscalar mediator. For light DM, mediator masses up to 100 (50) GeV are excluded for scalar (pseudoscalar) mediators. The result for the scalar mediator achieves some of the most stringent limits to date in this model.

Sirunyan, A. M., et al. (2018). "Pseudorapidity distributions of charged hadrons in proton-lead collisions at root s(NN)=5:02 and 8.16 TeV." Journal of High Energy Physics(1).
    The pseudorapidity distributions of charged hadrons in proton-lead collisions at nucleon-nucleon center-of-mass energies root s(NN) = 5.02 and 8.16 TeV are presented. The measurements are based on data samples collected by the CMS experiment at the LHC. The number of primary charged hadrons produced in non-single-diffractive proton-lead collisions is determined in the pseudorapidity range vertical bar eta(lab)vertical bar < 2.4. The charged-hadron multiplicity distributions are compared to the predictions from theoretical calculations and Monte Carlo event generators. In the center-of-mass pseudorapidity range vertical bar eta(cm)vertical bar < 0.5, the average charged-hadron multiplicity densities < dN(ch)/d eta(cm)>vertical bar(vertical bar eta cm vertical bar) < 0.5 are 17.1 +/- 0.01 (stat) +/- 0.59 (syst) and 20.10 +/- 0.01 (stat) +/- 0.5(syst) at root s(NN) = 5.02 and 8.16 TeV, respectively. The particle densities per participant nucleon are compared to similar measurements in proton-proton, proton-nucleus, and nucleus-nucleus collisions.

Sirunyan, A. M., et al. (2018). "Evidence for the Associated Production of a Single Top Quark and a Photon in Proton-Proton Collisions at root s=13 TeV." Physical Review Letters 121(22).
    The first evidence of events consistent with the production of a single top quark in association with a photon is reported. The analysis is based on proton-proton collisions at root s = 13 TeV and recorded by the CMS experiment in 2016, corresponding to an integrated luminosity of 35.9 fb(-1). Events are selected by requiring the presence of a muon (mu), a photon (gamma), an imbalance in transverse momentum from an undetected neutrino (nu), and at least two jets (j) of which exactly one is identified as associated with the hadronization of a b quark. A multivariate discriminant based on topological and kinematic event properties is employed to separate signal from background processes. An excess above the backgroundonly hypothesis is observed, with a significance of 4.4 standard deviations. A fiducial cross section is measured for isolated photons with transverse momentum greater than 25 GeV in the central region of the detector. The measured product of the cross section and branching fraction is sigma(pp -> t gamma j) B (t -> mu nu b) = 115 +/- 17 (stat) +/- 30(syst) fb, which is consistent with the standard model prediction.

Sirunyan, A. M., et al. (2018). "Performance of reconstruction and identification of tau leptons decaying to hadrons and nu(tau) in pp collisions at root s=13 TeV." Journal of Instrumentation 13.
    The algorithm developed by the CMS Collaboration to reconstruct and identify tau leptons produced in proton-proton collisions at root s = 7 and 8 TeV, via their decays to hadrons and a neutrino, has been significantly improved. The changes include a revised reconstruction of pi(0) candidates, and improvements in multivariate discriminants to separate tau leptons from jets and electrons. The algorithm is extended to reconstruct tau leptons in highly Lorentz-boosted pair production, and in the high-level trigger. The performance of the algorithm is studied using proton-proton collisions recorded during 2016 at root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). The performance is evaluated in terms of the efficiency for a genuine tau lepton to pass the identification criteria and of the probabilities for jets, electrons, and muons to be misidentified as tau leptons. The results are found to be very close to those expected from Monte Carlo simulation.

Sirunyan, A. M., et al. (2018). "Charged-particle nuclear modification factors in XeXe collisions at root S-NN=5.44 TeV." Journal of High Energy Physics(10).
    The differential yields of charged particles having pseudorapidity within vertical bar eta vertical bar < 1 are measured using xenon-xenon (XeXe) collisions at root S-NN = 5.44 TeV. The data, corresponding to an integrated luminosity of 3.42 mu b(-1), were collected in 2017 by the CMS experiment at the LHC. The yields are reported as functions of collision centrality and transverse momentum, pT, from 0.5 to 100 GeV. A previously reported pT spectrum from proton-proton collisions at root S = 5.02 TeV is used for comparison after correcting for the difference in center-of-mass energy. The nuclear modification factors using this reference, R-AA*, are constructed and compared to previous measurements and theoretical predictions. In head-on collisions, the R-AA* has a value of 0.17 in the pT range of 6-8 GeV, but increases to approximately 0.7 at 100 GeV. Above approximate to 6 GeV, the XeXe data show a notably smaller suppression than previous results for lead-lead (PbPb) collisions at root S-NN = 5.02 TeV when compared at the same centrality (i.e., the same fraction of total cross section). However, the XeXe suppression is slightly greater than that for PbPb in events having a similar number of participating nucleons.

Sirunyan, A. M., et al. (2018). "Constraining Gluon Distributions in Nuclei Using Dijets in Proton-Proton and Proton-Lead Collisions at root s(NN)=5.02 TeV." Physical Review Letters 121(6).
    The pseudorapidity distributions of dijets as functions of their average transverse momentum (p(T)(ave)) are measured in proton-lead (pPb) and proton-proton (pp) collisions. The data samples were collected by the CMS experiment at the CERN LHC, at a nucleon-nucleon center-of-mass energy of 5.02 TeV. A significant modification of the pPb spectra with respect to the pp spectra is observed in all p(T)(ave) intervals investigated. The ratios of the pPb and pp distributions are compared to next-to-leading order perturbative quantum chromodynamics calculations with unbound nucleon and nuclear parton distribution functions (PDFs). These results give the first evidence that the gluon PDF at large Bjorken x in lead ions is strongly suppressed with respect to the PDF in unbound nucleons.

Sirunyan, A. M., et al. (2018). "Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at root s=13 TeV." Physical Review D 98(3).
    The results of a previous search by the CMS Collaboration for squarks and gluinos are reinterpreted to constrain models of leptoquark (LQ) production. The search considers jets in association with a transverse momentum imbalance, using the M-T2 variable. The analysis uses proton-proton collision data at root s = 13 TeV, recorded with the CMS detector at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb(-1). Leptoquark pair production is considered with LQ decays to a neutrino and a top, bottom, or light quark. This reinterpretation considers higher mass values than the original CMS search to constrain both scalar and vector LQs. Limits on the cross section for LQ pair production are derived at the 95% confidence level depending on the LQ decay mode. A vector LQ decaying with a 50% branching fraction to t nu, and 50% to b tau, has been proposed as part of an explanation of anomalous flavor physics results. In such a model, using only the decays to t nu, LQ masses below 1530 GeV are excluded assuming the Yang-Mills case with coupling kappa = 1, or 1115 GeV in the minimal coupling case kappa = 0, placing the most stringent constraint to date from pair production of vector LQs.

Sirunyan, A. M., et al. (2018). "Event shape variables measured using multijet final states in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(12).
    The study of global event shape variables can provide sensitive tests of predictions for multijet production in proton-proton collisions. This paper presents a study of several event shape variables calculated using jet four momenta in proton-proton collisions at a centre-of-mass energy of 13 TeV and uses data recorded with the CMS detector at the LHC corresponding to an integrated luminosity of 2.2 fb(-1). After correcting for detector effects, the resulting distributions are compared with several theoretical predictions. The agreement generally improves as the energy, represented by the average transverse momentum of the two leading jets, increases.

Sirunyan, A. M., et al. (2018). "Measurement of the groomed jet mass in PbPb and pp collisions at root s(NN)=5:02 TeV." Journal of High Energy Physics(10).
    A measurement of the groomed jet mass in PbPb and pp collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV with the CMS detector at the LHC is presented. Jet grooming is a recursive procedure which sequentially removes soft constituents of a jet until a pair of hard subjets is found. The resulting groomed jets can be used to study modifications to the parton shower evolution in the presence of the hot and dense medium created in heavy ion collisions. Predictions of groomed jet properties from the pythia and herwig++ event generators agree with the measurements in pp collisions. When comparing the results from the most central PbPb collisions to pp data, a hint of an increase of jets with large jet mass is observed, which could originate from additional medium-induced radiation at a large angle from the jet axis. However, no modification of the groomed mass of the core of the jet is observed for all PbPb centrality classes. The PbPb results are also compared to predictions from the jewel and q-pythia event generators, which predict a large modification of the groomed mass not observed in the data.

Sirunyan, A. M., et al. (2018). "Measurement of the top quark mass with lepton plus jets final states using pp collisions at root s=13 TeV." European Physical Journal C 78(11).
    The mass of the top quark is measured using a sample of t (t) over bar events collected by the CMS detector using proton-proton collisions at root s = 13 TeV at the CERN LHC. Events are selected with one isolated muon or electron and at least four jets from data corresponding to an integrated luminosity of 35.9 fb(-1). For each event the mass is reconstructed from a kinematic fit of the decay products to a t (t) over bar hypothesis. Using the ideogram method, the top quark mass is determined simultaneously with an overall jet energy scale factor (JSF), constrained by the mass of the W boson in q (q) over bar' decays. The measurement is calibrated on samples simulated at next-to-leading order matched to a leadingorder parton shower. The top quark mass is found to be 172.25 +/- 0.08 (stat+JSF)+/- 0.62 (syst) GeV. The dependence of this result on the kinematic properties of the event is studied and compared to predictions of different models of t (t) over bar production, and no indications of a bias in the measurements are observed.

Sirunyan, A. M., et al. (2018). "Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton -proton collisions at=13 TeV." Journal of High Energy Physics(11).
    Measurements of the differential jet cross section are presented as a function of the jet mass in dijet events, in bins of jet transverse momentum, with and without a jet grooming algorithm. The data have been recorded by the CMS Collaboration in proton-proton collisions at the LHC at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 2.3 fb(-1). The absolute cross sections show slightly different jet transverse momentum spectra in data and Monte Carlo event generators for the settings used. Removing this transverse momentum dependence, the normalized cross section for ungroomed jets is consistent with the prediction from Monte Carlo event generators for masses below 30% of the transverse momentum. The normalized cross section for groomed jets is measured with higher precision than the ungroomed cross section. Semi-analytical calculations of the jet mass beyond leading logarithmic accuracy are compared to data, as well as predictions at leading order and next-to-leading order, which include parton showering and hadronization. Overall, in the normalized cross section, the theoretical predictions agree with the measured cross sections within the uncertainties for masses from 10 to 30% of the jet transverse momentum.

Sirunyan, A. M., et al. (2018). "Observation of (tt)over-barH Production." Physical Review Letters 120(23).
    The observation of Higgs boson production in association with a top quark-antiquark pair is reported, based on a combined analysis of proton-proton collision data at center-of-mass energies of root s = 7, 8, and 13 TeV, corresponding to integrated luminosities of up to 5.1, 19.7, and 35.9 fb(-1), respectively. The data were collected with the CMS detector at the CERN LHC. The results of statistically independent searches for Higgs bosons produced in conjunction with a top quark-antiquark pair and decaying to pairs of W bosons, Z bosons, photons, tau leptons, or bottom quark jets are combined to maximize sensitivity. An excess of events is observed, with a significance of 5.2 standard deviations, over the expectation from the background-only hypothesis. The corresponding expected significance from the standard model for a Higgs boson mass of 125.09 GeV is 4.2 standard deviations. The combined best fit signal strength normalized to the standard model prediction is 1.26(-0.26)(+0.31).

Sirunyan, A. M., et al. (2018). "Observation of Higgs Boson Decay to Bottom Quarks." Physical Review Letters 121(12).
    The observation of the standard model (SM) Higgs boson decay to a pair of bottom quarks is presented. The main contribution to this result is from processes in which Higgs bosons arc produced in association with a W or Z boson (VH), and are searched for in final states including 0, 1, or 2 charged leptons and two identified bottom quark jets. The results from the measurement of these processes in a data sample recorded by the CMS experiment in 2017, comprising 41.3 fb(-1) of proton-proton collisions at root s = 13 TeV, are described. When combined with previous VH measurements using data collected at root s = 7, 8, and 13 TeV, an excess of events is observed at m(H) = 125 GeV with a significance of 4.8 standard deviations, where the expectation for the SM Higgs boson is 4.9. The corresponding measured signal strength is 1.01 +/- 0.22. The combination of this result with searches by the CMS experiment for H -> b (b) over bar in other production processes yields an observed (expected) significance of 5.6 (5.5) standard deviations and a signal strength of 1.04 +/- 0.20.

Sirunyan, A. M., et al. (2018). "Observation of the chi(b1)(3P) and chi(b2)(3P) and Measurement of their Masses." Physical Review Letters 121(9).
    The chi(b1)(3P) and chi(b2)(3P) states are observed through their gamma(3S)(gamma) decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 80.0 fb(-1). The gamma(3S) mesons are identified through their dimuon decay channel, while the low-energy photons are detected after converting to e(+)e(-) pairs in the silicon tracker, leading to a chi(b)(3P) mass resolution of 2.2 MeV. This is the first time that the J = 1 and 2 states are well resolved and their masses individually measured: 10513.42 +/- 0.41(stat) +/- 0.18(syst) MeV and 10524.02 +/- 0.57(stat) +/- 0.18(syst) MeV; they are determined with respect to the world-average value of gamma(3S) mass, which has an uncertainty of 0.5 MeV. The mass splitting is measured to be 10.60 +/- 0.64(stat) +/- 0.17(syst) MeV.

Sirunyan, A. M., et al. (2018). "Search for a singly produced third-generation scalar leptoquark decaying to a tau lepton and a bottom quark in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(7).
    A search is presented for a singly produced third-generation scalar leptoquark decaying to a tau lepton and a bottom quark. Associated production of a leptoquark and a tau lepton is considered, leading to a final state with a bottom quark and two tau leptons. The search uses proton-proton collision data at a center-of-mass energy of 13 TeV recorded with the CMS detector, corresponding to an integrated luminosity of 35.9 fb(-1). Upper limits are set at 95% confidence level on the production cross section of the third-generation scalar leptoquarks as a function of their mass. From a comparison of the results with the theoretical predictions, a third-generation scalar leptoquark decaying to a tau lepton and a bottom quark, assuming unit Yukawa coupling (lambda), is excluded for masses below 740 GeV. Limits are also set on lambda of the hypothesized leptoquark as a function of its mass. Above lambda = 1.4, this result provides the best upper limit on the mass of a third-generation scalar leptoquark decaying to a tau lepton and a bottom quark.

Sirunyan, A. M., et al. (2018). "Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two tau leptons in proton-proton collisions at TeV." Journal of High Energy Physics(11).
    A search for exotic Higgs boson decays to light pseudoscalars in the final state of two muons and two tau leptons is performed using proton-proton collision data recorded by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV in 2016, corresponding to an integrated luminosity of 35.9 fb(-1). Masses of the pseudoscalar boson between 15.0 and 62.5 GeV are probed, and no significant excess of data is observed above the prediction of the standard model. Upper limits are set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different types of two-Higgs-doublet models extended with a complex scalar singlet.

Sirunyan, A. M., et al. (2018). "Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions a root s=13 TeVt." Journal of High Energy Physics(11).
    A search in energetic, high-multiplicity final states for evidence of physics beyond the standard model, such as black holes, string balls, and electroweak sphalerons, is presented. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) collected with the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV in 2016. Standard model backgrounds, dominated by multijet production, are determined from control regions in data without any reliance on simulation. No evidence for excesses above the predicted background is observed. Model-independent 95% confidence level upper limits on the cross section of beyond the standard model signals in these final states are set and further interpreted in terms of limits on semiclassical black hole, string ball, and sphaleron production. In the context of models with large extra dimensions, semiclassical black holes with minimum masses as high as 10.1 TeV and string balls with masses as high as 9.5 TeV are excluded by this search. Results of the first dedicated search for electroweak sphalerons are presented. An upper limit of 0.021 is set at 95% confidence level on the fraction of all quark-quark interactions above the nominal threshold energy of 9 TeV resulting in the sphaleron transition.

Sirunyan, A. M., et al. (2018). "Search for dark matter produced in association with a Higgs boson decaying to gamma gamma or tau(+)tau(-) at root s=13 TeV." Journal of High Energy Physics(9).
    A search for dark matter particles is performed by looking for events with large transverse momentum imbalance and a recoiling Higgs boson decaying to either a pair of photons or a pair of tau leptons. The search is based on proton-proton collision data at a center-of-mass energy of 13 TeV collected at the CERN LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb(-1). No significant excess over the expected standard model background is observed. Upper limits at 95% confidence level are presented for the product of the production cross section and branching fraction in the context of two benchmark simplified models. For the Z'-two-Higgs-doublet model (where Z' is a new massive boson mediator) with an intermediate heavy pseudoscalar particle of mass m(A) = 300 GeV and m(DM) = 100 GeV, the Z' masses from 550 GeV to 1265 GeV are excluded. For a baryonic Z' model, with m(DM) = 1 GeV, Z' masses up to 615 GeV are excluded. Results are also presented for the spin-independent cross section for the dark matter-nucleon interaction as a function of the mass of the dark matter particle. This is the first search for dark matter particles produced in association with a Higgs boson decaying to two tau leptons.

Sirunyan, A. M., et al. (2018). "Search for long-lived particles with displaced vertices in multijet events in proton-proton collisions at root s=13 TeV." Physical Review D 98(9).
    Results are reported from a search for long-lived particles in proton-proton collisions at root s = 13 TeV delivered by the CERN LHC and collected by the CMS experiment. The data sample, which was recorded during 2015 and 2016, corresponds to an integrated luminosity of 38.5 fb(-1). This search uses benchmark signal models in which long-lived particles are pair-produced and each decays into two or more quarks, leading to a signal with multiple jets and two displaced vertices composed of many tracks. No events with two well-separated high-track-multiplicity vertices are observed. Upper limits are placed on models of R-parity violating supersymmetry in which the long-lived particles are neutralinos or gluinos decaying solely into multijet final states or top squarks decaying solely into dijet final states. For neutralino, gluino, or top squark masses between 800 and 2600 GeV and mean proper decay lengths between 1 and 40 mm, the analysis excludes cross sections above 0.3 fb at 95% confidence level. Gluino and top squark masses are excluded below 2200 and 1400 GeV, respectively, for mean proper decay lengths between 0.6 and 80 mm. A method is provided for extending the results to other models with pair-produced long-lived particles.

Sirunyan, A. M., et al. (2018). "Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at root s=13 TeV." Physical Review D 98(11).
    A general search for the pair production of resonances, each decaying to two quarks, is reported. The search is conducted separately for heavier resonances (masses above 400 GeV), where each of the four final-state quarks generates a hadronic jet resulting in a four-jet signature, and for lighter resonances (masses between 80 and 400 GeV), where the pair of quarks from each resonance is collimated and reconstructed as a single jet resulting in a two-jet signature. In addition, a b-tagged selection is applied to target resonances with a bottom quark in the final state. The analysis uses data collected with the CMS detector at the CERN LHC, corresponding to an integrated luminosity of 35.9 fb(-1), from proton-proton collisions at a center-of-mass energy of 13 TeV. The mass spectra are analyzed for the presence of new resonances, and are found to be consistent with standard model expectations. The results are interpreted in the framework of R-parity-violating supersymmetry assuming the pair production of scalar top quarks decaying via the hadronic coupling lambda ''(312) or lambda ''(323) and upper limits on the cross section as a function of the top squark mass are set. These results probe a wider range of masses than previously explored at the LHC, and extend the top squark mass limits in the (t) over tilde -> qq' scenario.

Sirunyan, A. M., et al. (2018). "Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at root s=13 TeV." Physical Review D 98(9).
    A search for physics beyond the standard model is performed using a sample of high-mass diphoton events produced in proton-proton collisions at root s = 13 TeV. The data sample was collected in 2016 with the CMS detector at the LHC and corresponds to an integrated luminosity of 35.9 fb(-1). The search is performed for both resonant and nonresonant new physics signatures. At 95% confidence level, lower limits on the mass of the first Kaluza-Klein excitation of the graviton in the Randall-Sundrum warped extradimensional model are determined to be in the range of 2.3 to 4.6 TeV, for values of the associated coupling parameter between 0.01 and 0.2. Lower limits on the production of scalar resonances and modelindependent cross section upper limits are also provided. For the large extra-dimensional model of Arkani-amed, Dimopoulos, and Dvali, lower limits are set on the string mass scale M-S ranging from 5.6 to 9.7 TeV, depending on the model parameters. The first exclusion limits are set in the two-dimensional parameter space of a continuum clockwork model.

Sirunyan, A. M., et al. (2018). "Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at root 8 and 13 TeV." Journal of High Energy Physics(11).
    A search for resonances in the mass range 12-70 GeV produced in association with a b quark jet and a second jet, and decaying to a muon pair, is reported. The analysis is based on data from proton-proton collisions at center-of-mass energies of 8 and 13 TeV, collected with the CMS detector at the LHC and corresponding to integrated luminosities of 19.7 and 35.9 fb(-1), respectively. The search is carried out in two mutually exclusive event categories. Events in the first category are required to have a b quark jet in the central region (|| 2.4) and at least one jet in the forward region (|| > 2.4). Events in the second category are required to have two jets in the central region, at least one of which is identified as a b quark jet, no jets in the forward region, and low missing transverse momentum. An excess of events above the background near a dimuon mass of 28 GeV is observed in the 8 TeV data, corresponding to local significances of 4.2 and 2.9 standard deviations for the first and second event categories, respectively. A similar analysis conducted with the 13 TeV data results in a mild excess over the background in the first event category corresponding to a local significance of 2.0 standard deviations, while the second category results in a 1.4 standard deviation deficit. The fiducial cross section measurements and 95% confidence level upper limits on those for a resonance consistent with the 8 TeV excess are provided at both collision energies.

Sirunyan, A. M., et al. (2018). "Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at root s=13 TeV." Journal of High Energy Physics(11).
    A search for pair production of supersymmetric particles in events with two oppositely charged leptons (electrons or muons) and missing transverse momentum is reported. The data sample corresponds to an integrated luminosity of 35.9 fb(-1) of proton-proton collisions at TeV collected with the CMS detector during the 2016 data taking period at the LHC. No significant deviation is observed from the predicted standard model background. The results are interpreted in terms of several simplified models for chargino and top squark pair production, assuming R-parity conservation and with the neutralino as the lightest supersymmetric particle. When the chargino is assumed to undergo a cascade decay through sleptons, with a slepton mass equal to the average of the chargino and neutralino masses, exclusion limits at 95% confidence level are set on the masses of the chargino and neutralino up to 800 and 320 GeV, respectively. For top squark pair production, the search focuses on models with a small mass difference between the top squark and the lightest neutralino. When the top squark decays into an off-shell top quark and a neutralino, the limits extend up to 420 and 360 GeV for the top squark and neutralino masses, respectively.

Sirunyan, A. M., et al. (2018). "Studies of B-s2*(5840)(0) and B-s1(5830)(0) mesons including the observation of the B-s2*(5840)(0) -> (BKS0)-K-0 decay in proton- proton collisions at root s=8 TeV." European Physical Journal C 78(11).
    Measurements of B-s2*(5840)(0) and B-s1(5830)(0) mesons are performed using a data sample of proton-proton collisions corresponding to an integrated luminosity of 19.6 fb(-1), collected with the CMS detector at the LHC at a centre-of-mass energy of 8 TeV. The analysis studies P-wave B-s(0) meson decays into B(*)(+)K(-)and B(*)K-0(S)0, where the B+ and B-0 mesons are identified using the decays B+ -> J/psi K+ and B-0 -> J/psi K* (892)(0). The masses of the P-wave B-s(0) meson states are measured and the natural width of the B-s2*(5840)(0) state is determined. The first measurement of the mass difference between the charged and neutral B* mesons is also presented. The B-s2*(5840)(0) decay to (BKS0)-K-0 is observed, together with a measurement of its branching fraction relative to the B-s2*(5840)(0) -> B+K- decay.

Sirunyan, A. M., et al. (2018). "Azimuthal anisotropy of charged particles with transverse momentum up to 100GeV/c in PbPb collisions at root S-NN=5.02 TeV." Physics Letters B 776: 195-216.
    The Fourier coefficients v(2) and v(3) characterizing the anisotropy of the azimuthal distribution of charged particles produced in PbPb collisions at root S-NN = 5.02 TeV are measured with data collected by the CMS experiment. The measurements cover a broad transverse momentum range, 1 < p(T) < 100 GeV/c. The analysis focuses on the p(T) > 10 GeV/c range, where anisotropic azimuthal distributions should reflect the path-length dependence of parton energy loss in the created medium. Results are presented in several bins of PbPb collision centrality, spanning the 60% most central events. The v(2) coefficient is measured with the scalar product and the multiparticle cumulant methods, which have different sensitivities to initial-state fluctuations. The values from both methods remain positive up to p(T) similar to 60-80 GeV/c, in all examined centrality classes. The v(3) coefficient, only measured with the scalar product method, tends to zero for p(T) greater than or similar to 20 GeV/c. Comparisons between theoretical calculations and data provide new constraints on the path-length dependence of parton energy loss in heavy ion collisions and highlight the importance of the initial-state fluctuations. (C) 2017 The Author. Published by Elsevier B.V.

Sirunyan, A. M., et al. (2018). "Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at root s = 13 TeV (vol 9, 106, 2017)." Journal of High Energy Physics(1).
    
Sirunyan, A. M., et al. (2018). "Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at root s=8 TeV." Journal of High Energy Physics(3).
    Results are presented from a search for natural gauge-mediated supersymmetry (SUSY) in a scenario in which the top squark is the lightest squark, the next-to-lightest SUSY particle is a bino-like neutralino, and the lightest SUSY particle is the gravitino. The strong production of top squark pairs can produce events with pairs of top quarks and neutralinos, with each bino-like neutralino decaying to a photon and a gravitino. The search is performed using a sample of pp collision data accumulated by the CMS experiment at root s = 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The final state consists of a lepton (electron or muon), jets, and one or two photons. The imbalance in transverse momentum in the events is compared with the expected spectrum from standard model processes. No excess event yield is observed beyond the expected background, and the result is interpreted in the context of a general model of gauge-mediated SUSY breaking that leads to exclusion of top squark masses below 650-730 GeV.

Sirunyan, A. M., et al. (2018). "Search for vectorlike light-flavor quark partners in proton-proton collisions at root s=8 TeV." Physical Review D 97(7).
    A search is presented for heavy vectorlike quarks (VLQs) that couple only to light quarks in proton-proton collisions at root s = 8 TeV at the LHC. The data were collected by the CMS experiment during 2012 and correspond to an integrated luminosity of 19.7 fb(-1). Both single and pair production of VLQs are considered. The single-production search is performed for down-type VLQs (electric charge of magnitude 1/3), while the pair-production search is sensitive to up-type (charge of magnitude 2/3) and down-type VLQs. Final states with at least one muon or one electron are considered. No significant excess over standard model expectations is observed, and lower limits on the mass of VLQs are derived. The lower limits range from 400 to 1800 GeV, depending on the single-production cross section and the VLQ branching fractions B to W, Z, and Higgs bosons. When considering pair production alone, VLQs with masses below 845 GeV are excluded for B(W) = 1.0, and below 685 GeV for B(W) = 0.5, B(Z) = B(H) = 0.25. The results are more stringent than those previously obtained for single and pair production of VLQs coupled to light quarks.

Sirunyan, A. M., et al. (2018). "Study of dijet events with a large rapidity gap between the two leading jets in pp collisions at root s=7 TeV." European Physical Journal C 78(3).
    Events with no charged particles produced between the two leading jets are studied in proton-proton collisions at root s = 7 TeV. The jets were required to have transverse momentum p(T)(jet) > 40 GeV and pseudorapidity 1.5 < vertical bar eta(jet)vertical bar < 4.7, and to have values of eta(jet) with opposite signs. The data used for this study were collected with the CMSdetector during low-luminosity running at the LHC, and correspond to an integrated luminosity of 8 pb(-1). Events with no charged particles with p(T) > 0.2GeV in the interval -1 < eta < 1 between the jets are observed in excess of calculations that assume no color-singlet exchange. The fraction of events with such a rapidity gap, amounting to 0.5-1% of the selected dijet sample, is measured as a function of the pT of the second-leading jet and of the rapidity separation between the jets. The data are compared to previous measurements at the Tevatron, and to perturbative quantum chromodynamics calculations based on the Balitsky-Fadin-Kuraev-Lipatov evolution equations, including different models of the non-perturbative gap survival probability.

Sirunyan, A. M., et al. (2018). "Suppression of Excited gamma States Relative to the Ground State in Pb-Pb Collisions at root s(NN)=5.02 TeV." Physical Review Letters 120(14).
    The relative yields of gamma mesons produced in pp and Pb-Pb collisions at root s(NN) = 5.02 TeV and reconstructed via the dimuon decay channel are measured using data collected by the CMS experiment. Double ratios are formed by comparing the yields of the excited states, gamma(2S) and gamma(3S), to the ground state, gamma(1S), in both Pb-Pb and pp collisions at the same center-of-mass energy. The double ratios, [gamma(nS)/gamma(1S)](Pb-Pb)/[gamma(nS)/gamma(1S)](PP), are measured to be 0.308 +/- 0.055(stat) +/- 0.019(syst) for the gamma(2S) and less than 0.26 at 95% confidence level for the gamma(3S). No significant gamma(3S) signal is found in the Pb-Pb data. The double ratios are studied as a function of collision centrality, as well as gamma transverse momentum and rapidity. No significant dependencies are observed.

Sirunyan, A. M., et al. (2018). "Measurements of t(t)over-bar cross sections in association with b jets and inclusive jets and their ratio using dilepton final states in pp collisions at root s=13 TeV." Physics Letters B 776: 355-378.
    The cross sections for the production of t (t) over bar b (b) over bar and t (t) over bar jj events and their ratio sigma(t (t) over bar b (b) over bar)/sigma(t (t) over bar jj) are measured using data corresponding to an integrated luminosity of 2.3 fb(-1) collected in pp collisions at root s = 13 TeV with the CMS detector at the LHC. Events with two leptons (e or mu) and at least four reconstructed jets, including at least two identified as b quark jets, in the final state are selected. In the full phase space, the measured ratio is 0.022 +/- 0.003 (stat) +/- 0.006 (syst), the cross section sigma(t (t) over bar b (b) over bar) bis 4.0 +/- 0.6 (stat)+/- 1.3 (syst) pb and sigma(t (t) over bar jj) is 184 +/- 6 (stat)+/- 33 (syst) pb. The measurements are compared with the standard model expectations obtained from a POWHEG simulation at next-to-leading-order interfaced with PYTHIA. (c) 2017 The Author. Published by Elsevier B.V.

Tabanli, S., et al. (2018). "Broadband, White Light Emission from Doped and Undoped Insulators." Ecs Journal of Solid State Science and Technology 7(1): R3199-R3210.
    We present data on broadband, white light emission from insulating hosts under intense excitation in the near infrared in host materials that are undoped, partially-doped with rare earth ions, and that contain stoichiometric concentrations of rare earth ions. Much of the emission is found to have a blackbody-like structure in the visible and near infrared region. The origin of the emission as from a blackbody is also supported by the temporal characteristics of the emission in response to turning on and off the laser, and also by the dependence of the air pressure in the chamber. However, some of the data presented cannot be explained by blackbody emission alone, so other processes are proposed to explain the observed spectra. The role of the rare earth ion dopants in enhancing the broadband emission is also considered. (c) The Author(s) 2017. Published by ECS. All rights reserved.

Ulutas, K., et al. (2018). "Dielectric properties and conductivity of PVdF-co-HFP/LiClO4 polymer electrolytes." Canadian Journal of Physics 96(7): 786-791.
    In this study, it was aimed to prepare a series of PVdF-co-HFP based electrolytes with different LiClO4 loadings and to investigate their chemical and electrical properties in detail. For this purpose, PVdF-co-HFP based electrolytes with different LiClO4 loadings (1-20 weight %) were prepared using solution casting method. X-ray diffraction (XRD), differential scanning calorimetry, and thermogravimetric (TGA)-differential thermal and dielectric spectroscopy analysis of PVdF-co-HFP/LiClO4 were performed to characterize their structural, thermal, and dielectric properties, respectively. XRD results showed that the diffraction peaks of PVdF-co-HFP/LiClO4 electrolytes broadened and decreased with LiClO4. TGA patterns exhibited that PVdF-co-HFP/LiClO4 electrolytes with 20 wt % of LiClO4 had the lowest thermal stability and it degraded above 473 K, which is highly applicable for solid polymer electrolytes. Dielectric constant, dielectric loss, and conductivities were calculated by measuring capacitance and dielectric loss factor of PVdF-co-HFP/LiClO4 in the range from 10 mHz to 20 MHz frequencies at room temperature. In consequence, conductivities of PVdF-co-HFP/LiClO4 increased significantly with frequency for low loading of LiClO4 while they only slightly changed with higher LiClO4 addition. On the other hand, dielectric constant values of PVdF-co-HFP/LiClO4 films decreased with frequency whereas they rose with LiClO4 addition. The dielectric studies showed an increase in dielectric constant and dielectric loss with decreasing frequency. This result was attributed to high contribution of charge accumulation at the electrode-electrolyte interface. The electrolyte showed the maximum conductivity of 8 x 10(-2) S/cm at room temperature.

Yabas, E., et al. (2018). "Imidazole octasubstituted novel mono and double-decker phthalocyanines: Synthesis, characterization, electrical and gas sensing properties." Polyhedron 153: 51-63.
    Imidazole disubstituted phthalonitrile (1) was prepared by the reaction of 4,5-dichlorophthalonitrile with 4,5-diphenyl-1H-imidazolethiole. Imidazole octasubstituted metal free (2), zinc(II) (3), cobalt(II) (4) monophthalocyanines and lutetium(III) (5) and europium(III) (6) double-decker phthalocyanines were prepared by cyclotetramerization of compound 1. The new compounds were characterized by H-1 NMR, C-13 NMR, UV-vis, IR, MALDI-TOF mass, ESR spectra and elemental analysis. Dc and ac conductivity and gas sensing properties (at room temperature) of the compounds of 2-6 were studied between the temperatures of 295-523 K. Ac conductivity values of the films were measured in the frequency region of 40 Hz-100 kHz. The films were tested for the vapors of toluene, ethanol, THF, n-hexane, chloroform and xylene. DC conductivity results revealed that the compounds 2-6 show a semiconductor behavior. Results of ac measurements show dominant conduction mechanism can be modeled depending on temperature and frequency. The best sensitivity values were obtained for the xylene vapors. The sensor 3 showed best sensitivity among the other sensors for xylene vapor. Response times of the sensors were also determined. (C) 2018 Elsevier Ltd. All rights reserved.

Yavuz, I., et al. (2018). "Control of molecular dissociation by spatially inhomogeneous near fields." Physical Review A 98(4).
    Tailored intense laser fields can be used to steer electron and nuclear dynamics in molecules and control chemical reactions. Here we demonstrate that inhomogeneous nanoscopic near fields provide an additional mechanism for controlling light-induced chemical reactions. This is investigated by quantum-dynamical calculations on dissociation of H-2(+) in few-cycle near fields with a controlled carrier-envelope phase. Directional dissociation asymmetry analysis reveals that the spatial asymmetry of the field is critical in controlling and in modifying field-induced dissociation pathways such as zero-photon dissociation, bond softening, and above-threshold dissociation. The degree of impact strongly depends on the maximum length scale of coherent control in a dissociation channel. The results pave the way towards coherent control of molecular reactions in a wide range of molecules in inhomogeneous near fields.



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