1e:I[23489,["/_next/static/immutable/chunks/0cmb0ng968nlp.js","/_next/static/immutable/chunks/1c7dg80qt12uw.js","/_next/static/immutable/chunks/2bmdwv49ba1qx.js","/_next/static/immutable/chunks/3ld61_1ghpsxn.js"],"ShareMenu"] 1f:I[55078,["/_next/static/immutable/chunks/0cmb0ng968nlp.js","/_next/static/immutable/chunks/1c7dg80qt12uw.js","/_next/static/immutable/chunks/2bmdwv49ba1qx.js","/_next/static/immutable/chunks/3ld61_1ghpsxn.js"],"AuthorMetricsPanel"] 20:I[39060,["/_next/static/immutable/chunks/0cmb0ng968nlp.js","/_next/static/immutable/chunks/1c7dg80qt12uw.js","/_next/static/immutable/chunks/2bmdwv49ba1qx.js","/_next/static/immutable/chunks/3ld61_1ghpsxn.js"],"AuthorPapers"] 3e:I[49310,["/_next/static/immutable/chunks/0cmb0ng968nlp.js","/_next/static/immutable/chunks/1c7dg80qt12uw.js"],"IconMark"] 21:T486,The CMS apparatus was identified, a few years before the start of the LHC operation at CERN, to feature properties well suited to particle-flow (PF) reconstruction: a highly-segmented tracker, a fine-grained electromagnetic calorimeter, a hermetic hadron calorimeter, a strong magnetic field, and an excellent muon spectrometer.A fully-fledged PF reconstruction algorithm tuned to the CMS detector was therefore developed and has been consistently used in physics analyses for the first time at a hadron collider.For each collision, the comprehensive list of final-state particles identified and reconstructed by the algorithm provides a global event description that leads to unprecedented CMS performance for jet and hadronic τ decay reconstruction, missing transverse momentum determination, and electron and muon identification.This approach also allows particles from pileup interactions to be identified and enables efficient pileup mitigation methods.The data collected by CMS at a centre-of-mass energy of 8 TeV show excellent agreement with the simulation and confirm the superior PF performance at least up to an average of 20 pileup interactions.22:T4f6,Results on two-particle angular correlations for charged particles emitted in pPb collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV are presented. The analysis uses two million collisions collected with the CMS detector at the LHC. The correlations are studied over a broad range of pseudorapidity, eta, and full azimuth, phi, as a function of charged particle multiplicity and particle transverse momentum, pt. In high-multiplicity events, a long-range (2 < abs(Delta(eta)) < 4), near-side (Delta(phi) approximately 0) structure emerges in the two-particle Delta(eta)-Delta(phi) correlation functions. This is the first observation of such correlations in proton-nucleus collisions, resembling the ridge-like correlations seen in high-multiplicity pp collisions at sqrt(s) = 7 TeV and in AA collisions over a broad range of center-of-mass energies. The correlation strength exhibits a pronounced maximum in the range of pt = 1-1.5 GeV and an approximately linear increase with charged particle multiplicity for high-multiplicity events. These observations are qualitatively similar to those in pp collisions when selecting the same observed particle multiplicity, while the overall strength of the correlations is significantly larger in pPb collisions.23:T4f5,Properties of the Higgs boson with mass near 125[Formula: see text] are measured in proton-proton collisions with the CMS experiment at the LHC. Comprehensive sets of production and decay measurements are combined. The decay channels include [Formula: see text], [Formula: see text], [Formula: see text], [Formula: see text], [Formula: see text], and [Formula: see text] pairs. The data samples were collected in 2011 and 2012 and correspond to integrated luminosities of up to 5.1[Formula: see text] at 7[Formula: see text] and up to 19.7[Formula: see text] at 8[Formula: see text]. From the high-resolution [Formula: see text] and [Formula: see text] channels, the mass of the Higgs boson is determined to be [Formula: see text]. For this mass value, the event yields obtained in the different analyses tagging specific decay channels and production mechanisms are consistent with those expected for the standard model Higgs boson. The combined best-fit signal relative to the standard model expectation is [Formula: see text] at the measured mass. The couplings of the Higgs boson are probed for deviations in magnitude from the standard model predictions in multiple ways, including searches for invisible and undetected decays. No significant deviations are found.24:T499,A bstract A detailed description is reported of the analysis used by the CMS Collaboration in the search for the standard model Higgs boson in pp collisions at the LHC, which led to the observation of a new boson. The data sample corresponds to integrated luminosities up to 5.1 fb −1 at $ \sqrt{s}=7 $ TeV, and up to 5.3 fb −1 at $ \sqrt{s}=8 $ TeV . The results for five Higgs boson decay modes γγ , ZZ, WW, ττ , and bb, which show a combined local significance of 5 standard deviations near 125 GeV, are reviewed. A fit to the invariant mass of the two high resolution channels, γγ and ZZ → 4 ℓ , gives a mass estimate of 125 . 3 ± 0 . 4 (stat.) ± 0 . 5 (syst.) GeV. The measurements are interpreted in the context of the standard model Lagrangian for the scalar Higgs field interacting with fermions and vector bosons. The measured values of the corresponding couplings are compared to the standard model predictions. The hypothesis of custodial symmetry is tested through the measurement of the ratio of the couplings to the W and Z bosons. All the results are consistent, within their uncertainties, with the expectations for a standard model Higgs boson.25:T417,New sets of parameters ("tunes") for the underlying-event (UE) modelling of the pythia8, pythia6 and herwig++ Monte Carlo event generators are constructed using different parton distribution functions. Combined fits to CMS UE proton-proton ([Formula: see text]) data at [Formula: see text] and to UE proton-antiproton ([Formula: see text]) data from the CDF experiment at lower [Formula: see text], are used to study the UE models and constrain their parameters, providing thereby improved predictions for proton-proton collisions at 13[Formula: see text]. In addition, it is investigated whether the values of the parameters obtained from fits to UE observables are consistent with the values determined from fitting observables sensitive to double-parton scattering processes. Finally, comparisons are presented of the UE tunes to "minimum bias" (MB) events, multijet, and Drell-Yan ([Formula: see text] lepton-antilepton+jets) observables at 7 and 8[Formula: see text], as well as predictions for MB and UE observables at 13[Formula: see text].26:T614,Many measurements and searches for physics beyond the standard model at the LHC rely on the efficient identification of heavy-flavour jets, i.e. jets originating from bottom or charm quarks.In this paper, the discriminating variables and the algorithms used for heavy-flavour jet identification during the first years of operation of the CMS experiment in proton-proton collisions at a centre-of-mass energy of 13 TeV, are presented.Heavy-flavour jet identification algorithms have been improved compared to those used previously at centre-of-mass energies of 7 and 8 TeV.For jets with transverse momenta in the range expected in simulated t t events, these new developments result in an efficiency of 68% for the correct identification of a b jet for a probability of 1% of misidentifying a light-flavour jet.The improvement in relative efficiency at this misidentification probability is about 15%, compared to previous CMS algorithms.In addition, for the first time algorithms have been developed to identify jets containing two b hadrons in Lorentz-boosted event topologies, as well as to tag c jets.The large data sample recorded in 2016 at a centre-of-mass energy of 13 TeV has also allowed the development of new methods to measure the efficiency and misidentification probability of heavy-flavour jet identification algorithms.The b jet identification efficiency is measured with a precision of a few per cent at moderate jet transverse momenta (between 30 and 300 GeV) and about 5% at the highest jet transverse momenta (between 500 and 1000 GeV).27:Td79,Combined analysis of proton-proton collision data from the Large Hadron Collider at CERN by the CMS and LHCb collaborations leads to the observation of the extremely rare decay of the strange B meson into muons; the result is compatible with the standard model of particle physics, and does not show any signs of new physics, such as supersymmetry. When searching for physics beyond the standard model of particle physics, one promising route is to consider processes at very high energies that can be produced in particle colliders. Here, the CMS and LHCb collaborations working at the Large Hadron Collider at CERN, the largest particle accelerator in the world, report the observation of the extremely rare decay of a B meson into muons. In this decay, discrepancies from the standard model predictions might point towards supersymmetry which is thought to be a plausible candidate for a theory beyond the standard model. The combined results from the CMS and LHCb collaborations, however, confirm the standard model and do not show any signs of supersymmetry. The restart of the Large Hadron Collider this spring with higher operation energies will increase the production rate of B mesons and might bring new surprises and constraints for theories beyond the standard model of particle physics. The standard model of particle physics describes the fundamental particles and their interactions via the strong, electromagnetic and weak forces. It provides precise predictions for measurable quantities that can be tested experimentally. The probabilities, or branching fractions, of the strange B meson ( ) and the B0 meson decaying into two oppositely charged muons (μ+ and μ−) are especially interesting because of their sensitivity to theories that extend the standard model. The standard model predicts that the and decays are very rare, with about four of the former occurring for every billion mesons produced, and one of the latter occurring for every ten billion B0 mesons1. A difference in the observed branching fractions with respect to the predictions of the standard model would provide a direction in which the standard model should be extended. Before the Large Hadron Collider (LHC) at CERN2 started operating, no evidence for either decay mode had been found. Upper limits on the branching fractions were an order of magnitude above the standard model predictions. The CMS (Compact Muon Solenoid) and LHCb (Large Hadron Collider beauty) collaborations have performed a joint analysis of the data from proton–proton collisions that they collected in 2011 at a centre-of-mass energy of seven teraelectronvolts and in 2012 at eight teraelectronvolts. Here we report the first observation of the µ+µ− decay, with a statistical significance exceeding six standard deviations, and the best measurement so far of its branching fraction. Furthermore, we obtained evidence for the µ+µ− decay with a statistical significance of three standard deviations. Both measurements are statistically compatible with standard model predictions and allow stringent constraints to be placed on theories beyond the standard model. The LHC experiments will resume taking data in 2015, recording proton–proton collisions at a centre-of-mass energy of 13 teraelectronvolts, which will approximately double the production rates of and B0 mesons and lead to further improvements in the precision of these crucial tests of the standard model.28:T5ba,The properties of a Higgs boson candidate are measured in the $H\ensuremath{\rightarrow}ZZ\ensuremath{\rightarrow}4\ensuremath{\ell}$ decay channel, with $\ensuremath{\ell}=e$, $\ensuremath{\mu}$, using data from $pp$ collisions corresponding to an integrated luminosity of $5.1\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ at the center-of-mass energy of $\sqrt{s}=7\text{ }\text{ }\mathrm{TeV}$ and $19.7\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}\text{1}}$ at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$, recorded with the CMS detector at the LHC. The new boson is observed as a narrow resonance with a local significance of 6.8 standard deviations, a measured mass of $125.6\ifmmode\pm\else\textpm\fi{}0.4(\text{stat})\ifmmode\pm\else\textpm\fi{}0.2(\text{syst})\text{ }\text{ }\mathrm{GeV}$, and a total width $\ensuremath{\le}3.4\text{ }\text{ }\mathrm{GeV}$ at the 95% confidence level. The production cross section of the new boson times its branching fraction to four leptons is measured to be ${0.93}_{\ensuremath{-}0.23}^{+0.26}{(\text{stat})}_{\ensuremath{-}0.09}^{+0.13}(\text{syst})$ times that predicted by the standard model. Its spin-parity properties are found to be consistent with the expectations for the standard-model Higgs boson. The hypotheses of a pseudoscalar and all tested spin-1 boson hypotheses are excluded at the 99% confidence level or higher. All tested spin-2 boson hypotheses are excluded at the 95% confidence level or higher.29:T59d,Measurements of two- and four-particle angular correlations for charged particles emitted in pPb collisions are presented over a wide range in pseudorapidity and full azimuth. The data, corresponding to an integrated luminosity of approximately 31nb−1, were collected during the 2013 LHC pPb run at a nucleon–nucleon center-of-mass energy of 5.02 TeV by the CMS experiment. The results are compared to 2.76 TeV semi-peripheral PbPb collision data, collected during the 2011 PbPb run, covering a similar range of particle multiplicities. The observed correlations are characterized by the near-side (|Δϕ|≈0) associated pair yields and the azimuthal anisotropy Fourier harmonics (vn). The second-order (v2) and third-order (v3) anisotropy harmonics are extracted using the two-particle azimuthal correlation technique. A four-particle correlation method is also applied to obtain the value of v2 and further explore the multi-particle nature of the correlations. Both associated pair yields and anisotropy harmonics are studied as a function of particle multiplicity and transverse momentum. The associated pair yields, the four-particle v2, and the v3 become apparent at about the same multiplicity. A remarkable similarity in the v3 signal as a function of multiplicity is observed between the pPb and PbPb systems. Predictions based on the color glass condensate and hydrodynamic models are compared to the experimental results.2a:T4f8,Measurements of two- and multi-particle angular correlations in pp collisions at s = 5 , 7 , and 13 TeV are presented as a function of charged-particle multiplicity. The data, corresponding to integrated luminosities of 1.0 pb − 1 (5 TeV), 6.2 pb − 1 (7 TeV), and 0.7 pb − 1 (13 TeV), were collected using the CMS detector at the LHC. The second-order ( v 2 ) and third-order ( v 3 ) azimuthal anisotropy harmonics of unidentified charged particles, as well as v 2 of K S 0 and Λ / Λ ‾ particles, are extracted from long-range two-particle correlations as functions of particle multiplicity and transverse momentum. For high-multiplicity pp events, a mass ordering is observed for the v 2 values of charged hadrons (mostly pions), K S 0 , and Λ / Λ ‾ , with lighter particle species exhibiting a stronger azimuthal anisotropy signal below p T ≈ 2 GeV/ c . For 13 TeV data, the v 2 signals are also extracted from four- and six-particle correlations for the first time in pp collisions, with comparable magnitude to those from two-particle correlations. These observations are similar to those seen in pPb and PbPb collisions, and support the interpretation of a collective origin for the observed long-range correlations in high-multiplicity pp collisions.2b:T510,New sets of CMS underlying-event parameters ("tunes") are presented for the pythia8 event generator. These tunes use the NNPDF3.1 parton distribution functions (PDFs) at leading (LO), next-to-leading (NLO), or next-to-next-to-leading (NNLO) orders in perturbative quantum chromodynamics, and the strong coupling evolution at LO or NLO. Measurements of charged-particle multiplicity and transverse momentum densities at various hadron collision energies are fit simultaneously to determine the parameters of the tunes. Comparisons of the predictions of the new tunes are provided for observables sensitive to the event shapes at LEP, global underlying event, soft multiparton interactions, and double-parton scattering contributions. In addition, comparisons are made for observables measured in various specific processes, such as multijet, Drell-Yan, and top quark-antiquark pair production including jet substructure observables. The simulation of the underlying event provided by the new tunes is interfaced to a higher-order matrix-element calculation. For the first time, predictions from pythia8 obtained with tunes based on NLO or NNLO PDFs are shown to reliably describe minimum-bias and underlying-event data with a similar level of agreement to predictions from tunes using LO PDF sets.2c:T686,The study of the spin-parity and tensor structure of the interactions of the recently discovered Higgs boson is performed using the $H\ensuremath{\rightarrow}ZZ,Z{\ensuremath{\gamma}}^{*},{\ensuremath{\gamma}}^{*}{\ensuremath{\gamma}}^{*}\ensuremath{\rightarrow}4\ensuremath{\ell}$, $H\ensuremath{\rightarrow}WW\ensuremath{\rightarrow}\ensuremath{\ell}\ensuremath{\nu}\ensuremath{\ell}\ensuremath{\nu}$, and $H\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma}$ decay modes. The full data set recorded by the CMS experiment during the LHC run 1 is used, corresponding to an integrated luminosity of up to $5.1\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ at a center-of-mass energy of 7 TeV and up to $19.7\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ at 8 TeV. A wide range of spin-two models is excluded at a 99% confidence level or higher, or at a 99.87% confidence level for the minimal gravitylike couplings, regardless of whether assumptions are made on the production mechanism. Any mixed-parity spin-one state is excluded in the $ZZ$ and $WW$ modes at a greater than 99.999% confidence level. Under the hypothesis that the resonance is a spin-zero boson, the tensor structure of the interactions of the Higgs boson with two vector bosons $ZZ$, $Z\ensuremath{\gamma}$, $\ensuremath{\gamma}\ensuremath{\gamma}$, and $WW$ is investigated and limits on eleven anomalous contributions are set. Tighter constraints on anomalous $HVV$ interactions are obtained by combining the $HZZ$ and $HWW$ measurements. All observations are consistent with the expectations for the standard model Higgs boson with the quantum numbers ${J}^{\mathrm{PC}}={0}^{++}$.2d:T42f,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 are 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 sqrt[s]=13 TeV, are described. When combined with previous VH measurements using data collected at sqrt[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→bb[over ¯] in other production processes yields an observed (expected) significance of 5.6 (5.5) standard deviations and a signal strength of 1.04±0.20.2e:T5b5,Results are presented from a search for the rare decays ${B}_{s}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ and ${B}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ in $pp$ collisions at $\sqrt{s}=7$ and 8 TeV, with data samples corresponding to integrated luminosities of 5 and $20\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$, respectively, collected by the CMS experiment at the LHC. An unbinned maximum-likelihood fit to the dimuon invariant mass distribution gives a branching fraction $\mathcal{B}({B}_{s}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}})=({3.0}_{\ensuremath{-}0.9}^{+1.0})\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}9}$, where the uncertainty includes both statistical and systematic contributions. An excess of ${B}_{s}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ events with respect to background is observed with a significance of 4.3 standard deviations. For the decay ${B}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ an upper limit of $\mathcal{B}({B}^{0}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}})<1.1\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}9}$ at the 95% confidence level is determined. Both results are in agreement with the expectations from the standard model.2f:T427,Abstract A search for the standard model Higgs boson decaying to a W-boson pair at the LHC is reported. The event sample corresponds to an integrated luminosity of 4.9 fb−1and 19.4 fb−1collected with the CMS detector in pp collisions at $ \sqrt{s} $ = 7 and 8 TeV, respectively. The Higgs boson candidates are selected in events with two or three charged leptons. An excess of events above background is observed, consistent with the expectation from the standard model Higgs boson with a mass of around 125 GeV. The probability to observe an excess equal or larger than the one seen, under the background-only hypothesis, corresponds to a significance of 4.3 standard deviations formH= 125.6 GeV. The observed signal cross section times the branching fraction to WW formH= 125.6 GeV is $ 0.72_{-0.18}^{+0.20 } $ times the standard model expectation. The spin-parityJP= 0+hypothesis is favored against a narrow resonance withJP= 2+orJP= 0−that decays to a W-boson pair. This result provides strong evidence for a Higgs-like boson decaying to a W-boson pair.30:T4f5,At the start of Run 2 in 2015, the LHC delivered proton-proton collisions at a center-of-mass energy of 13\TeV. During Run 2 (years 2015–2018) the LHC eventually reached a luminosity of 2.1× 10$^{34}$ cm$^{-2}$s$^{-1}$, almost three times that reached during Run 1 (2009–2013) and a factor of two larger than the LHC design value, leading to events with up to a mean of about 50 simultaneous inelastic proton-proton collisions per bunch crossing (pileup). The CMS Level-1 trigger was upgraded prior to 2016 to improve the selection of physics events in the challenging conditions posed by the second run of the LHC. This paper describes the performance of the CMS Level-1 trigger upgrade during the data taking period of 2016–2018. The upgraded trigger implements pattern recognition and boosted decision tree regression techniques for muon reconstruction, includes pileup subtraction for jets and energy sums, and incorporates pileup-dependent isolation requirements for electrons and tau leptons. In addition, the new trigger calculates high-level quantities such as the invariant mass of pairs of reconstructed particles. The upgrade reduces the trigger rate from background processes and improves the trigger efficiency for a wide variety of physics signals.31:T48b,Abstract The measurement of the luminosity recorded by the CMS detector installed at LHC interaction point 5, using proton–proton collisions at $$\sqrt{s}=13\,{\text {TeV}} $$ s = 13 TeV in 2015 and 2016, is reported. The absolute luminosity scale is measured for individual bunch crossings using beam-separation scans (the van der Meer method), with a relative precision of 1.3 and 1.0% in 2015 and 2016, respectively. The dominant sources of uncertainty are related to residual differences between the measured beam positions and the ones provided by the operational settings of the LHC magnets, the factorizability of the proton bunch spatial density functions in the coordinates transverse to the beam direction, and the modeling of the effect of electromagnetic interactions among protons in the colliding bunches. When applying the van der Meer calibration to the entire run periods, the integrated luminosities when CMS was fully operational are 2.27 and 36.3 $$\,\text {fb}^{-1}$$ fb - 1 in 2015 and 2016, with a relative precision of 1.6 and 1.2%, respectively. These are among the most precise luminosity measurements at bunched-beam hadron colliders.32:T546,The suppression of the individual $\ensuremath{\Upsilon}(nS)$ states in PbPb collisions with respect to their yields in $pp$ data has been measured. The PbPb and $pp$ data sets used in the analysis correspond to integrated luminosities of $150\text{ }\text{ }\ensuremath{\mu}{\mathrm{b}}^{\ensuremath{-}1}$ and $230\text{ }\text{ }{\mathrm{nb}}^{\ensuremath{-}1}$, respectively, collected in 2011 by the CMS experiment at the LHC, at a center-of-mass energy per nucleon pair of 2.76 TeV. The $\ensuremath{\Upsilon}(nS)$ yields are measured from the dimuon invariant mass spectra. The suppression of the $\ensuremath{\Upsilon}(nS)$ yields in PbPb relative to the yields in $pp$, scaled by the number of nucleon-nucleon collisions, ${R}_{AA}$, is measured as a function of the collision centrality. Integrated over centrality, the ${R}_{AA}$ values are $0.56\ifmmode\pm\else\textpm\fi{}0.08(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}0.07(\mathrm{syst})$, $0.12\ifmmode\pm\else\textpm\fi{}0.04(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}0.02(\mathrm{syst})$, and lower than 0.10 (at 95% confidence level), for the $\ensuremath{\Upsilon}(1S)$, $\ensuremath{\Upsilon}(2S)$, and $\ensuremath{\Upsilon}(3S)$ states, respectively. The results demonstrate the sequential suppression of the $\ensuremath{\Upsilon}(nS)$ states in PbPb collisions at LHC energies.33:T5d3,The second-order azimuthal anisotropy Fourier harmonics, v2, are obtained in p-Pb and PbPb collisions over a wide pseudorapidity (η) range based on correlations among six or more charged particles. The p-Pb data, corresponding to an integrated luminosity of 35 nb-1, were collected during the 2013 LHC p-Pb run at a nucleon-nucleon center-of-mass energy of 5.02 TeV by the CMS experiment. A sample of semiperipheral PbPb collision data at √sNN=2.76 TeV, corresponding to an integrated luminosity of 2.5 μb-1 and covering a similar range of particle multiplicities as the p-Pb data, is also analyzed for comparison. The six- and eight-particle cumulant and the Lee-Yang zeros methods are used to extract the v2 coefficients, extending previous studies of two- and four-particle correlations. For both the p-Pb and PbPb systems, the v2 values obtained with correlations among more than four particles are consistent with previously published four-particle results. These data support the interpretation of a collective origin for the previously observed long-range (large Δη) correlations in both systems. The ratios of v2 values corresponding to correlations including different numbers of particles are compared to theoretical predictions that assume a hydrodynamic behavior of a p-Pb system dominated by fluctuations in the positions of participant nucleons. These results provide new insights into the multiparticle dynamics of collision systems with a very small overlapping region.34:T534,Abstract The performance is presented of the reconstruction and identification algorithms for electrons and photons with the CMS experiment at the LHC. The reported results are based on proton-proton collision data collected at a center-of-mass energy of 13 TeV and recorded in 2016–2018, corresponding to an integrated luminosity of 136 fb^-1. Results obtained from lead-lead collision data collected at √(sNN)=5.02 TeV are also presented. Innovative techniques are used to reconstruct the electron and photon signals in the detector and to optimize the energy resolution. Events with electrons and photons in the final state are used to measure the energy resolution and energy scale uncertainty in the recorded events. The measured energy resolution for electrons produced in Z boson decays in proton-proton collision data ranges from 2 to 5%, depending on electron pseudorapidity and energy loss through bremsstrahlung in the detector material. The energy scale in the same range of energies is measured with an uncertainty smaller than 0.1 (0.3)% in the barrel (endcap) region in proton-proton collisions and better than 1 (3)% in the barrel (endcap) region in heavy ion collisions. The timing resolution for electrons from Z boson decays with the full 2016–2018 proton-proton collision data set is measured to be 200 ps.35:T51a,A search for invisible decays of a Higgs boson is performed using proton-proton collision data collected with the CMS detector at the LHC in 2016 at a center-of-mass energy √ s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb -1 .The search targets the production of a Higgs boson via vector boson fusion.The data are found to be in agreement with the background contributions from standard model processes.An observed (expected) upper limit of 0.33 (0.25), at 95% confidence level, is placed on the branching fraction of the Higgs boson decay to invisible particles, assuming standard model production rates and a Higgs boson mass of 125.09GeV.Results from a combination of this analysis and other direct searches for invisible decays of the Higgs boson, performed using data collected at √ s = 7, 8, and 13 TeV, are presented.An observed (expected) upper limit of 0.19 (0.15), at 95% confidence level, is set on the branching fraction of invisible decays of the Higgs boson.The combined limit represents the most stringent bound on the invisible branching fraction of the Higgs boson reported to date.This result is also interpreted in the context of Higgs-portal dark matter models, in which upper bounds are placed on the spin-independent dark-matter-nucleon scattering cross section.36:T556,Abstract Measurements from the CMS experiment at the LHC of dihadron correlations for charged particles produced in PbPb collisions at a nucleon–nucleon centre-of-mass energy of 2.76 TeV are presented. The results are reported as a function of the particle transverse momenta (pT) and collision centrality over a broad range in relative pseudorapidity (Δη) and the full range of relative azimuthal angle (Δϕ). The observed two-dimensional correlation structure in Δη and Δϕ is characterised by a narrow peak at (Δη,Δϕ)≈(0,0) from jet-like correlations and a long-range structure that persists up to at least |Δη|=4. An enhancement of the magnitude of the short-range jet peak is observed with increasing centrality, especially for particles of pT around 1–2 GeV/c. The long-range azimuthal dihadron correlations are extensively studied using a Fourier decomposition analysis. The extracted Fourier coefficients are found to factorise into a product of single-particle azimuthal anisotropies up to pT≈3–3.5 GeV/c for at least one particle from each pair, except for the second-order harmonics in the most central PbPb events. Various orders of the single-particle azimuthal anisotropy harmonics are extracted for associated particle pT of 1–3 GeV/c, as a function of the trigger particle pT up to 20 GeV/c and over the full centrality range.37:T42a,A search for the standard model Higgs boson ($H$) decaying to $b\overline{b}$ when produced in association with a weak vector boson ($V$) is reported for the following channels: $W(\ensuremath{\mu}\ensuremath{\nu})H$, $W(e\ensuremath{\nu})H$, $W(\ensuremath{\tau}\ensuremath{\nu})H$, $Z(\ensuremath{\mu}\ensuremath{\mu})H$, $Z(ee)H$, and $Z(\ensuremath{\nu}\ensuremath{\nu})H$. The search is performed in data samples corresponding to integrated luminosities of up to 5.1 inverse femtobarns at $\sqrt{s}=7\text{ }\text{ }\mathrm{TeV}$ and up to $18.9\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$, recorded by the CMS experiment at the LHC. An excess of events is observed above the expected background with a local significance of 2.1 standard deviations for a Higgs boson mass of 125 GeV, consistent with the expectation from the production of the standard model Higgs boson. The signal strength corresponding to this excess, relative to that of the standard model Higgs boson, is $1.0\ifmmode\pm\else\textpm\fi{}0.5$.38:T455,The spectra of charged particles produced within the pseudorapidity window |η| < 1 at √ s NN = 5.02 TeV are measured using 404 µb -1 of PbPb and 27.4 pb -1 of pp data collected by the CMS detector at the LHC in 2015.The spectra are presented over the transverse momentum ranges spanning 0.5 < p T < 400 GeV in pp and 0.7 < p T < 400 GeV in PbPb collisions.The corresponding nuclear modification factor, R AA , is measured in bins of collision centrality.The R AA in the 5% most central collisions shows a maximal suppression by a factor of 7-8 in the p T region of 6-9 GeV.This dip is followed by an increase, which continues up to the highest p T measured, and approaches unity in the vicinity of p T = 200 GeV.The R AA is compared to theoretical predictions and earlier experimental results at lower collision energies.The newly measured pp spectrum is combined with the pPb spectrum previously published by the CMS collaboration to construct the pPb nuclear modification factor, R pA , up to 120 GeV.For p T > 20 GeV, R pA exhibits weak momentum dependence and shows a moderate enhancement above unity.39:T466,Abstract Results of searches for heavy stable charged particles produced in pp collisions at $ \sqrt{s} $ = 7 and 8 TeV are presented corresponding to an integrated luminosity of 5.0 fb−1 and 18.8 fb−1, respectively. Data collected with the CMS detector are used to study the momentum, energy deposition, and time-of-flight of signal candidates. Leptons with an electric charge between e/3 and 8e, as well as bound states that can undergo charge exchange with the detector material, are studied. Analysis results are presented for various combinations of signatures in the inner tracker only, inner tracker and muon detector, and muon detector only. Detector signatures utilized are long time-of-flight to the outer muon system and anomalously high (or low) energy deposition in the inner tracker. The data are consistent with the expected background, and upper limits are set on the production cross section of long-lived gluinos, scalar top quarks, and scalar τ leptons, as well as pair produced long-lived leptons. Corresponding lower mass limits, ranging up to 1322 GeV/c2 for gluinos, are the most stringent to date.3a:T513,Abstract Properties of the Higgs boson are measured in the H → ZZ → 4ℓ (ℓ = e,μ) decay channel. A data sample of proton-proton collisions at $$ \sqrt{s}=13 $$ s=13 TeV, collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 35.9 fb−1is used. The signal strength modifierμ, defined as the ratio of the observed Higgs boson rate in the H → ZZ → 4ℓ decay channel to the standard model expectation, is measured to beμ = 1.05− 0.17+ 0.19atmH= 125.09 GeV, the combined ATLAS and CMS measurement of the Higgs boson mass. The signal strength modifiers for the individual Higgs boson production modes are also measured. The cross section in the fiducial phase space defined by the requirements on lepton kinematics and event topology is measured to be 2. 92− 0.44+ 0.48(stat)− 0.24+ 0.28(syst)fb, which is compatible with the standard model prediction of 2.76 ± 0.14 fb. Differential cross sections are reported as a function of the transverse momentum of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet. The Higgs boson mass is measured to bemH= 125.26 ± 0.21 GeV and the width is constrained using the on-shell invariant mass distribution to be ΓH< 1.10 GeV, at 95% confidence level.3b:T434,Abstract A search has been made for events containing an energetic jet and an imbalance in transverse momentum using a data sample of pp collisions at a center-of-mass energy of 7 TeV. This signature is common to both dark matter and extra dimensions models. The data were collected by the CMS detector at the LHC and correspond to an integrated luminosity of 5.0 fb−1. The number of observed events is consistent with the standard model expectation. Constraints on the dark matter-nucleon scattering cross sections are determined for both spin-independent and spin-dependent interaction models. For the spin-independent model, these are the most constraining limits for a dark matter particle with mass below 3.5 GeV/c 2, a region unexplored by direct detection experiments. For the spin-dependent model, these are the most stringent constraints over the 0.1–200 GeV/c 2 mass range. The constraints on the Arkani-Hamed, Dimopoulos, and Dvali model parameter M D determined as a function of the number of extra dimensions are also an improvement over the previous results.3c:T563,Evidence for the light-by-light scattering process, γ γ → γ γ , in ultraperipheral PbPb collisions at a centre-of-mass energy per nucleon pair of 5.02 TeV is reported. The analysis is conducted using a data sample corresponding to an integrated luminosity of 390 μ b − 1 recorded by the CMS experiment at the LHC. Light-by-light scattering processes are selected in events with two photons exclusively produced, each with transverse energy E T γ > 2 GeV , pseudorapidity | η γ | < 2.4 , diphoton invariant mass m γ γ > 5 GeV , diphoton transverse momentum p T γ γ < 1 GeV , and diphoton acoplanarity below 0.01. After all selection criteria are applied, 14 events are observed, compared to expectations of 9.0 ± 0.9 (theo) events for the signal and 4.0 ± 1.2 (stat) for the background processes. The excess observed in data relative to the background-only expectation corresponds to a significance of 3.7 standard deviations, and has properties consistent with those expected for the light-by-light scattering signal. The measured fiducial light-by-light scattering cross section, σ fid ( γ γ → γ γ ) = 120 ± 46 (stat) ± 28 (syst) ± 12 (theo) nb , is consistent with the standard model prediction. The m γ γ distribution is used to set new exclusion limits on the production of pseudoscalar axion-like particles, via the process, in the mass range .16:["$","div",null,{"className":"mx-auto max-w-6xl px-4 py-6 sm:px-6 sm:py-10","children":[["$","header",null,{"className":"grid gap-6 lg:grid-cols-[1fr_22rem] lg:items-end","children":[["$","div",null,{"children":[["$","p",null,{"className":"label mb-2 text-accent","children":["Researcher profile · ","OpenAlex"]}],["$","h1",null,{"className":"text-3xl font-bold sm:text-4xl","children":"M. 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The search is performed in five decay modes: gamma gamma, ZZ, WW, tau tau, and b b-bar. An excess of events is observed above the expected background, with a local significance of 5.0 standard deviations, at a mass near 125 GeV, signalling the production of a new particle. The expected significance for a standard model Higgs boson of that mass is 5.8 standard deviations. The excess is most significant in the two decay modes with the best mass resolution, gamma gamma and ZZ; a fit to these signals gives a mass of 125.3 +/- 0.4 (stat.) +/- 0.5 (syst.) GeV. The decay to two photons indicates that the new particle is a boson with spin different from one.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"E. Aguiló","id":"openalex:A5056886475","orcid":"https://orcid.org/0000-0002-7171-3812","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Dragicevic","id":"openalex:A5086528441","orcid":"https://orcid.org/0000-0003-1967-6783","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. Erö","id":"openalex:A5113501345","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"Christian W. Fabjan","id":"openalex:A5108086684","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Friedl","id":"openalex:A5102904489","orcid":"https://orcid.org/0000-0002-7420-2559","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"Rudolf Konrad Fruhwirth","id":"openalex:A5027832388","orcid":"https://orcid.org/0000-0002-0054-3369","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"V. M. Ghete","id":"openalex:A5073746799","orcid":"https://orcid.org/0000-0002-9595-6560","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. Hammer","id":"openalex:A5108098225","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"Michael J. R. Hoch","id":"openalex:A5103042749","orcid":"https://orcid.org/0000-0002-4690-1993","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"N. Hörmann","id":"openalex:A5112601085","orcid":"https://orcid.org/0000-0001-6944-5575","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. 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Waltenberger","id":"openalex:A5009221549","orcid":"https://orcid.org/0000-0002-6215-7228","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"G. Walzel","id":"openalex:A5054156640","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"E. Widl","id":"openalex:A5049342015","orcid":"https://orcid.org/0000-0002-2834-306X","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"C.-E. Wulz","id":"openalex:A5108167515","orcid":"https://orcid.org/0000-0001-9226-5812","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"V. A. Chekhovsky","id":"openalex:A5090149024","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"I. Emeliantchik","id":"openalex:A5012227044","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"A. Litomin","id":"openalex:A5107931385"},{"name":"В. 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Stefanovitch","id":"openalex:A5111949749","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. Suarez Gonzalez","id":"openalex:A5107843080","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"A. Fedorov","id":"openalex:A5107902977"},{"name":"M. Korzhik","id":"openalex:A5113915436","orcid":"https://orcid.org/0000-0001-8334-1502","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"O. 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Bansal","id":"openalex:A5000721235","orcid":"https://orcid.org/0000-0003-1992-0336","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"W. Beaumont","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Cornelis","id":"openalex:A5018937696","orcid":"https://orcid.org/0000-0001-9502-5363","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"E. A. 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Caudron","id":"openalex:A5105784401","affiliation":"UCLouvain","institutionId":"I95674353","institutionUrl":"https://ror.org/02495e989","affiliations":["Université Catholique de Louvain , Louvain-la-Neuve , Belgium","Université Catholique de Louvain, Louvain-la-Neuve, Belgium"]}],"venue":"Journal of Instrumentation","venueId":"S116045149","publisher":"Institute of Physics","publisherId":"P4310311669","year":2017,"publishedDate":"2017-10-06","type":"article","citationCount":981,"referenceCount":61,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1088/1748-0221/12/10/p10003","oaUrl":"https://iopscience.iop.org/article/10.1088/1748-0221/12/10/P10003/pdf","pdfUrl":"https://iopscience.iop.org/article/10.1088/1748-0221/12/10/P10003/pdf","topics":[{"id":"T11044","name":"Particle Detector Development and Performance","score":0.8500999808311462,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":0.13979999721050262,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10527","name":"High-Energy Particle Collisions Research","score":0.0027000000700354576,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W2624881227"},{"ids":{"openalex":"W2566668505","doi":"10.1088/1748-0221/12/01/p01020"},"title":"The CMS trigger system","abstract":"This paper describes the CMS trigger system and its performance during Run 1 of the LHC.The trigger system consists of two levels designed to select events of potential physics interest from a GHz (MHz) interaction rate of proton-proton (heavy ion) collisions.The first level of the trigger is implemented in hardware, and selects events containing detector signals consistent with an electron, photon, muon, τ lepton, jet, or missing transverse energy.A programmable menu of up to 128 object-based algorithms is used to select events for subsequent processing.The trigger thresholds are adjusted to the LHC instantaneous luminosity during data taking in order to restrict the output rate to 100 kHz, the upper limit imposed by the CMS readout electronics.The second level, implemented in software, further refines the purity of the output stream, selecting an average rate of 400 Hz for offline event storage.The objectives, strategy and performance of the trigger system during the LHC Run 1 are described.","authors":[{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute , Yerevan , Armenia","Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute , Yerevan , Armenia","Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Institut für Hochenergiephysik der OeAW , Wien , Austria","Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute , Yerevan , Armenia","Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"E. Asilar","id":"openalex:A5007914806","orcid":"https://orcid.org/0000-0001-5680-599X","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute , Yerevan , Armenia","Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. 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Bakhshiansohi","id":"openalex:A5035613981","orcid":"https://orcid.org/0000-0001-5741-3357","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University , Ghent , Belgium","Université Catholique de Louvain, Louvain-la-Neuve, Belgium"]}],"venue":"Journal of Instrumentation","venueId":"S116045149","publisher":"Institute of Physics","publisherId":"P4310311669","year":2018,"publishedDate":"2018-05-08","type":"article","citationCount":632,"referenceCount":75,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1088/1748-0221/13/05/p05011","oaUrl":"https://iopscience.iop.org/article/10.1088/1748-0221/13/05/P05011/pdf","pdfUrl":"https://iopscience.iop.org/article/10.1088/1748-0221/13/05/P05011/pdf","topics":[{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":0.7842000126838684,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T11044","name":"Particle Detector Development and Performance","score":0.1923000067472458,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10527","name":"High-Energy Particle Collisions Research","score":0.00570000009611249,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W2777349738"},{"ids":{"openalex":"W2797305656","doi":"10.1088/1748-0221/13/06/p06015"},"title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √ s =13 TeV","abstract":"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 √ 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.","authors":[{"name":"A. 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Beluffi","id":"openalex:A5109854725","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University , Ghent , Belgium","UCLouvain, Louvain-la-Neuve, Belgium"]}],"venue":"Physics Letters B","venueId":"S173952182","publisher":"Elsevier BV","publisherId":"P4310320990","year":2013,"publishedDate":"2013-06-25","type":"article","citationCount":488,"referenceCount":60,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1016/j.physletb.2013.06.028","oaUrl":"https://www.sciencedirect.com/science/article/pii/S0370269313005030/pdfft?md5=20d4d6c2dd8e5013cc2d4e782f4056dd&pid=1-s2.0-S0370269313005030-main.pdf","pdfUrl":"https://www.sciencedirect.com/science/article/pii/S0370269313005030/pdfft?md5=20d4d6c2dd8e5013cc2d4e782f4056dd&pid=1-s2.0-S0370269313005030-main.pdf","topics":[{"id":"T10527","name":"High-Energy Particle Collisions Research","score":0.9984999895095825,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10224","name":"Quantum Chromodynamics and Particle Interactions","score":0.00019999999494757503,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":0.00009999999747378752,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W1529468456"},{"ids":{"openalex":"W2145474863","doi":"10.1140/epjc/s10052-014-3076-z","pmid":"25814871"},"title":"Observation of the diphoton decay of the Higgs boson and measurement of its properties","abstract":"Observation of the diphoton decay mode of the recently discovered Higgs boson and measurement of some of its properties are reported. The analysis uses the entire dataset collected by the CMS experiment in proton-proton collisions during the 2011 and 2012 LHC running periods. The data samples correspond to integrated luminosities of 5.1[Formula: see text]at [Formula: see text] and 19.7[Formula: see text]at 8[Formula: see text] . A clear signal is observed in the diphoton channel at a mass close to 125[Formula: see text] with a local significance of [Formula: see text], where a significance of [Formula: see text] is expected for the standard model Higgs boson. The mass is measured to be [Formula: see text] , and the best-fit signal strength relative to the standard model prediction is [Formula: see text][Formula: see text][Formula: see text]. Additional measurements include the signal strength modifiers associated with different production mechanisms, and hypothesis tests between spin-0 and spin-2 models.","authors":[{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. 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Additional results are given for various assumptions on the scaling behavior of the production and decay modes, including generic parametrizations based on ratios of cross sections and branching fractions or couplings. The results are compatible with the standard model predictions in all parametrizations considered. In addition, constraints are placed on various two Higgs doublet models.","authors":[{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"F. Ambrogi","id":"openalex:A5107897710","orcid":"https://orcid.org/0000-0002-9486-0444","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"E. Asilar","id":"openalex:A5007914806","orcid":"https://orcid.org/0000-0001-5680-599X","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"T. 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The data were collected by the CMS detector in proton-proton collisions at the LHC and correspond to an integrated luminosity of 19.7[Formula: see text]at a centre-of-mass energy of 8[Formula: see text]. The number of observed events is found to be consistent with the standard model prediction. Limits are placed on the DM-nucleon scattering cross section as a function of the DM particle mass for spin-dependent and spin-independent interactions. Limits are also placed on the scale parameter [Formula: see text] in the Arkani-Hamed, Dimopoulos, and Dvali (ADD) model of large extra dimensions, and on the unparticle model parameter [Formula: see text]. The constraints on ADD models and unparticles are the most stringent limits in this channel and those on the DM-nucleon scattering cross section are an improvement over previous collider results.","authors":[{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. 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Ocampo Rios","id":"openalex:A5106305906","orcid":"https://orcid.org/0009-0002-1506-515X","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"D. Ryckbosch","id":"openalex:A5042370486","orcid":"https://orcid.org/0000-0002-8759-7553","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"S. Salva Diblen","id":"openalex:A5113496429","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"M. Sigamani","id":"openalex:A5107844255","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"Nadja Strobbe","id":"openalex:A5031258898","orcid":"https://orcid.org/0000-0001-8835-8282","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"F. Thyssen","id":"openalex:A5112603787","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]}],"venue":"The European Physical Journal C","venueId":"S94052278","publisher":"Springer Science+Business Media","publisherId":"P4310319900","year":2015,"publishedDate":"2015-05-01","type":"article","citationCount":393,"referenceCount":87,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1140/epjc/s10052-015-3451-4","oaUrl":"https://doi.org/10.1140/epjc/s10052-015-3451-4","topics":[{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":0.9932000041007996,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T11090","name":"Dark Matter and Cosmic Phenomena","score":0.004699999932199717,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T11044","name":"Particle Detector Development and Performance","score":0.0005000000237487257,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W2799676946"},{"ids":{"openalex":"W1968635670","doi":"10.1103/physrevlett.110.081803","pmid":"23473131"},"title":"Study of the Mass and Spin-Parity of the Higgs Boson Candidate via Its Decays to Z Boson Pairs","abstract":"A study is presented of the mass and spin-parity of the new boson recently observed at the LHC at a mass near 125 GeV. An integrated luminosity of $17.3\\text{ }\\text{ }{\\mathrm{fb}}^{\\ensuremath{-}1}$, collected by the CMS experiment in proton-proton collisions at center-of-mass energies of 7 and 8 TeV, is used. The measured mass in the $ZZ$ channel, where both $Z$ bosons decay to $e$ or $\\ensuremath{\\mu}$ pairs, is $126.2\\ifmmode\\pm\\else\\textpm\\fi{}0.6(\\mathrm{stat})\\ifmmode\\pm\\else\\textpm\\fi{}0.2(\\mathrm{syst})\\text{ }\\text{ }\\mathrm{GeV}$. The angular distributions of the lepton pairs in this channel are sensitive to the spin-parity of the boson. Under the assumption of spin 0, the present data are consistent with the pure scalar hypothesis, while disfavoring the pure pseudoscalar hypothesis.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"E. Aguiló","id":"openalex:A5056886475","orcid":"https://orcid.org/0000-0002-7171-3812","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. 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Sirunyan","id":"openalex:A5107826728","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW , Wien , Austria","European Organization for Nuclear Research, Geneva, Switzerland"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW , Wien , Austria","European Organization for Nuclear Research, Geneva, Switzerland"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"A. 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The analyzed data sample corresponds to an integrated luminosity of 1.14 fb(-1). In this search, a kinematic variable α(T) is used as the main discriminator between events with genuine and misreconstructed missing transverse energy. No excess of events over the standard model expectation is found. Exclusion limits in the parameter space of the constrained minimal supersymmetric extension of the standard model are set. In this model, squark masses below 1.1 TeV are excluded at 95% C.L. Gluino masses below 1.1 TeV are also ruled out at 95% C.L. for values of the universal scalar mass parameter below 500 GeV.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. 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Yazgan","id":"openalex:A5088249841","orcid":"https://orcid.org/0000-0001-5732-7950","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"Nikolaos Zaganidis","id":"openalex:A5107826097","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"Suzan Basegmez du Pree","id":"openalex:A5107916218","orcid":"https://orcid.org/0000-0003-1599-6974","affiliation":"UCLouvain","institutionId":"I95674353","institutionUrl":"https://ror.org/02495e989","affiliations":["Université Catholique de Louvain, Louvain-la-Neuve, Belgium"]}],"venue":"Physical Review Letters","venueId":"S24807848","publisher":"American Physical Society","publisherId":"P4310320261","year":2015,"publishedDate":"2015-06-29","type":"article","citationCount":276,"referenceCount":56,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1103/physrevlett.115.012301","oaUrl":"http://link.aps.org/pdf/10.1103/PhysRevLett.115.012301","pdfUrl":"http://link.aps.org/pdf/10.1103/PhysRevLett.115.012301","topics":[{"id":"T10527","name":"High-Energy Particle Collisions Research","score":0.9990000128746033,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10224","name":"Quantum Chromodynamics and Particle Interactions","score":0.00009999999747378752,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":0.00009999999747378752,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W2153692276"},{"ids":{"openalex":"W2596459038","doi":"10.1007/jhep05(2012)063"},"title":"Suppression of non-prompt J/ψ, prompt J/ψ, and $ \\Upsilon $(1S) in PbPb collisions at $ \\sqrt {{{s_{\\text{NN}}}}} = 2.76 $ TeV","abstract":"Abstract Yields of prompt and non-prompt J/ψ, as well as $ \\Upsilon $ (1S) mesons, are measured by the CMS experiment via their μ + μ − decays in PbPb and pp collisions at $ \\sqrt {{{s_{\\text{NN}}}}} = 2.76 $ TeV for quarkonium rapidity |y| < 2.4. Differential cross sections and nuclear modification factors are reported as functions of y and transverse momentum p T, as well as collision centrality. For prompt J/ψ with relatively high p T (6.5 < p T < 30 GeV/c), a strong, centrality-dependent suppression is observed in PbPb collisions, compared to the yield in pp collisions scaled by the number of inelastic nucleon-nucleon collisions. In the same kinematic range, a suppression of non-prompt J/ψ, which is sensitive to the in-medium b-quark energy loss, is measured for the first time. Also the low-p T $ \\Upsilon $ (1S) mesons are suppressed in PbPb collisions.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Dragicevic","id":"openalex:A5086528441","orcid":"https://orcid.org/0000-0003-1967-6783","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. Erö","id":"openalex:A5113501345","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"Christian W. Fabjan","id":"openalex:A5108086684","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Friedl","id":"openalex:A5102904489","orcid":"https://orcid.org/0000-0002-7420-2559","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"R. Frühwirth","id":"openalex:A5106826073","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"V. M. 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Results are based on a sample of proton-proton collision data collected at center-of-mass energy [Formula: see text] with the CMS detector in 2012, corresponding to an integrated luminosity of 19.5 [Formula: see text]. The observed event rates are in agreement with expectations from the standard model. These results probe charginos and neutralinos with masses up to 720 [Formula: see text], and sleptons up to 260 [Formula: see text], depending on the model details.","authors":[{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. 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The data sample is divided into three jet multiplicity categories (3-5, 6-7, and 8 or more jets), and studied further in bins of two variables: the scalar sum of jet transverse momenta and the missing transverse momentum. The observed numbers of events in various categories are consistent with backgrounds expected from standard model processes. Exclusion limits are presented for several simplified supersymmetric models of squark or gluino pair production.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Dragicevic","id":"openalex:A5086528441","orcid":"https://orcid.org/0000-0003-1967-6783","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. Erö","id":"openalex:A5113501345","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"Christian W. 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A data sample corresponding to an integrated luminosity of 150 μb−1 is analyzed. Jets are reconstructed using combined information from tracking and calorimetry, using the anti-kT algorithm with R=0.3. The dijet momentum balance and angular correlations are studied as a function of collision centrality and leading jet transverse momentum. For the most peripheral PbPb collisions, good agreement of the dijet momentum balance distributions with pp data and reference calculations at the same collision energy is found, while more central collisions show a strong imbalance of leading and subleading jet transverse momenta attributed to the jet-quenching effect. The dijets in central collisions are found to be more unbalanced than the reference, for leading jet transverse momenta up to the highest values studied.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. 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The elliptic anisotropy parameter, ${v}_{2}$, defined as the second coefficient in a Fourier expansion of the particle invariant yields, is extracted using the event-plane method, two- and four-particle cumulants, and Lee-Yang zeros. The anisotropy is presented as a function of transverse momentum (${p}_{\\mathrm{T}}$), pseudorapidity ($\\ensuremath{\\eta}$) over a broad kinematic range, $0.3<{p}_{\\mathrm{T}}<20$ GeV/c, $|\\ensuremath{\\eta}|<2.4$, and in 12 classes of collision centrality from 0 to $80%$. The results are compared to those obtained at lower center-of-mass energies, and various scaling behaviors are examined. When scaled by the geometric eccentricity of the collision zone, the elliptic anisotropy is found to obey a universal scaling with the transverse particle density for different collision systems and center-of-mass energies.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Dragicevic","id":"openalex:A5086528441","orcid":"https://orcid.org/0000-0003-1967-6783","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. Erö","id":"openalex:A5113501345","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"Christian W. Fabjan","id":"openalex:A5108086684","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Friedl","id":"openalex:A5102904489","orcid":"https://orcid.org/0000-0002-7420-2559","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"R. 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The dataset corresponds to an integrated luminosity of 4.9 inverse femtobarns at a centre-of-mass energy of 7 TeV and 19.7 inverse femtobarns at 8 TeV. Each tau lepton decays hadronically or leptonically to an electron or a muon, leading to six different final states for the tau-lepton pair, all considered in this analysis. An excess of events is observed over the expected background contributions, with a local significance larger than 3 standard deviations for m[H] values between 115 and 130 GeV. The best fit of the observed H to tau tau signal cross section for m[H] = 125 GeV is 0.78 +- 0.27 times the standard model expectation. These observations constitute evidence for the 125 GeV Higgs boson decaying to a pair of tau leptons.","authors":[{"name":"S. Chatrchyan","id":"openalex:A5107933385","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"M. Dragicevic","id":"openalex:A5086528441","orcid":"https://orcid.org/0000-0003-1967-6783","affiliation":"Austrian Academy of Sciences","institutionId":"I138211613","institutionUrl":"https://ror.org/03anc3s24","affiliations":["Institut für Hochenergiephysik der OeAW, Wien, Austria"]},{"name":"J. 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Thyssen","id":"openalex:A5112603787","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"M. Tytgat","id":"openalex:A5107027924","orcid":"https://orcid.org/0000-0002-3990-2074","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"S. Walsh","id":"openalex:A5107392555","orcid":"https://orcid.org/0000-0003-1689-2309","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]},{"name":"E. Yazgan","id":"openalex:A5088249841","orcid":"https://orcid.org/0000-0001-5732-7950","affiliation":"Ghent University","institutionId":"I32597200","institutionUrl":"https://ror.org/00cv9y106","affiliations":["Ghent University, Ghent, Belgium"]}],"venue":"Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields","venueId":"S4210190737","publisher":"American Physical Society","publisherId":"P4310320261","year":2014,"publishedDate":"2014-01-21","type":"article","citationCount":256,"referenceCount":64,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1103/physrevd.89.012003","oaUrl":"http://link.aps.org/pdf/10.1103/PhysRevD.89.012003","pdfUrl":"http://link.aps.org/pdf/10.1103/PhysRevD.89.012003","topics":[{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":1,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10224","name":"Quantum Chromodynamics and Particle Interactions","score":0,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T11044","name":"Particle Detector Development and Performance","score":0,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W2102671432"},{"ids":{"openalex":"W2125007678","doi":"10.1140/epjc/s10052-015-3709-x","pmid":"26640401"},"title":"Measurement of the differential cross section for top quark pair production in pp collisions at $$\\sqrt{s} = 8\\,\\text {TeV} $$ s = 8 TeV","abstract":"The normalized differential cross section for top quark pair ([Formula: see text]) production is measured in pp collisions at a centre-of-mass energy of 8[Formula: see text] at the CERN LHC using the CMS detector in data corresponding to an integrated luminosity of 19.7[Formula: see text]. The measurements are performed in the lepton[Formula: see text]jets ([Formula: see text][Formula: see text]jets) and in the dilepton ([Formula: see text], [Formula: see text], and [Formula: see text]) decay channels. The [Formula: see text] cross section is measured as a function of the kinematic properties of the charged leptons, the jets associated to b quarks, the top quarks, and the [Formula: see text] system. The data are compared with several predictions from perturbative quantum chromodynamic up to approximate next-to-next-to-leading-order precision. No significant deviations are observed relative to the standard model predictions.","authors":[{"name":"V. Khachatryan","id":"openalex:A5005250779","orcid":"https://orcid.org/0000-0003-2567-2930","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik der OeAW, Vienna, Austria"]},{"name":"T. 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Bruno","id":"openalex:A5104240200","orcid":"https://orcid.org/0000-0001-8857-8197","affiliation":"UCLouvain","institutionId":"I95674353","institutionUrl":"https://ror.org/02495e989","affiliations":["Université Catholique de Louvain, Louvain-la-Neuve, Belgium"]}],"venue":"Journal of High Energy Physics","venueId":"S187585107","publisher":"Springer Nature","publisherId":"P4310319965","year":2017,"publishedDate":"2017-11-01","type":"article","citationCount":236,"referenceCount":79,"isOpenAccess":true,"sourceUrl":"https://doi.org/10.1007/jhep11(2017)047","oaUrl":"https://doi.org/10.1007/jhep11(2017)047","topics":[{"id":"T10048","name":"Particle physics theoretical and experimental studies","score":1,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T10224","name":"Quantum Chromodynamics and Particle Interactions","score":0,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"},{"id":"T11044","name":"Particle Detector Development and Performance","score":0,"subfieldId":"3106","subfield":"Nuclear and High Energy Physics","fieldId":"31","field":"Physics and Astronomy"}],"sources":["openalex"],"id":"openalex:W2729360300"},{"ids":{"openalex":"W2743153918","doi":"10.1016/j.physletb.2018.02.004"},"title":"Observation of the Higgs boson decay to a pair of τ leptons with the CMS detector","abstract":"A measurement of the H → τ τ 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 13 TeV . The data set corresponds to an integrated luminosity of 35.9 fb − 1 . The H → τ τ 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 → τ τ signal production cross section and branching fraction is 1.09 − 0.26 + 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 τ leptons by a single experiment.","authors":[{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"F. Ambrogi","id":"openalex:A5107897710","orcid":"https://orcid.org/0000-0002-9486-0444","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"E. 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The analysis is based on events with energy deposits in the forward calorimeters, which cover pseudorapidities of −6 . 6 < η < −3 . 0 and +3 . 0 < η < +5 . 2. An inelastic cross section of 68 . 6 ± 0 . 5(syst) ± 1 . 6(lumi) mb is obtained for events with M X > 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.","authors":[{"name":"A. M. Sirunyan","id":"openalex:A5107826728","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"A. Tumasyan","id":"openalex:A5069509278","orcid":"https://orcid.org/0009-0000-0684-6742","affiliation":"A. Alikhanyan National Laboratory","institutionId":"I132091411","institutionUrl":"https://ror.org/00ad27c73","affiliations":["Yerevan Physics Institute, Yerevan, Armenia"]},{"name":"W. Adam","id":"openalex:A5074924703","orcid":"https://orcid.org/0000-0001-9099-4341","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"F. Ambrogi","id":"openalex:A5107897710","orcid":"https://orcid.org/0000-0002-9486-0444","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"E. Asilar","id":"openalex:A5007914806","orcid":"https://orcid.org/0000-0001-5680-599X","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"T. Bergauer","id":"openalex:A5114334441","orcid":"https://orcid.org/0000-0002-5786-0293","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"J. Brandstetter","id":"openalex:A5107411550","orcid":"https://orcid.org/0000-0003-3881-976X","affiliation":"Institute of High Energy Physics","institutionId":"I4210129701","institutionUrl":"https://ror.org/039shy520","affiliations":["Institut für Hochenergiephysik, Wien, Austria"]},{"name":"E. 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