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741 result(s) for "D. Liko"
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Measurement of the differential t t ¯ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks
A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton + jets channel of top quark pair production ( ) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than 400 . The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of 138 . The differential production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of .
Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at ... TeV
An analysis of dijet events in PbPb and pp collisions is performed to explore the properties of energy loss by partons traveling in a quark-gluon plasma. Data are collected at a nucleon-nucleon center-of-mass energy of 2.76 TeV at the LHC. The distribution of transverse momentum (p sub(T)) surrounding dijet systems is measured by selecting charged particles in different ranges of p sub(T) and at different angular cones of pseudorapidity and azimuth. The measurement is performed as a function of centrality of the PbPb collisions, the p sub(T) asymmetry of the jets in the dijet pair, and the distance parameter R used in the anti-k sub(T) jet clustering algorithm. In events with unbalanced dijets, PbPb collisions show an enhanced multiplicity in the hemisphere of the subleading jet, with the p sub(T) imbalance compensated by an excess of low-p sub(T) particles at large angles from the jet axes. [Figure not available: see fulltext.]
Azimuthal correlations in Z +jets events in proton–proton collisions at $$\\sqrt{s} = 13\\,\\text {Te}\\hspace{-.08em}\\text {V}
The production of Z bosons associated with jets is measured in $$\\text {p}\\text {p}$$ pp collisions at $$\\sqrt{s}=13\\,\\text {Te}\\hspace{-.08em}\\text {V} $$ s = 13 Te V with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 $$\\,\\text {fb}^{-1}$$ fb - 1 . The multiplicity of jets with transverse momentum $$p_{\\textrm{T}} > 30\\,\\text {Ge}\\hspace{-.08em}\\text {V} $$ p T > 30 Ge V is measured for different regions of the Z boson’s $$p_{\\textrm{T}} (\\text {Z })$$ p T ( Z ) , from lower than 10 $$\\,\\text {Ge}\\hspace{-.08em}\\text {V}$$ Ge V to higher than 100 $$\\,\\text {Ge}\\hspace{-.08em}\\text {V}$$ Ge V . The azimuthal correlation $$\\varDelta \\phi $$ Δ ϕ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $$p_{\\textrm{T}} (\\text {Z })$$ p T ( Z ) . The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $$p_{\\textrm{T}} (\\text {Z })$$ p T ( Z ) regions.
Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at ... TeV by the CMS and TOTEM experiments
(ProQuest: ... denotes formulae and/or non-USASCII text omitted; see image).Pseudorapidity (...) distributions of charged particles produced in proton-proton collisions at a centre-of-mass energy of 8... are measured in the ranges ... and ... covered by the CMS and TOTEM detectors, respectively. The data correspond to an integrated luminosity of ... ... Measurements are presented for three event categories. The most inclusive category is sensitive to 91-96 % of the total inelastic proton-proton cross section. The other two categories are disjoint subsets of the inclusive sample that are either enhanced or depleted in single diffractive dissociation events. The data are compared to models used to describe high-energy hadronic interactions. None of the models considered provide a consistent description of the measured distributions.
Search for a light charged Higgs boson decaying to ... in pp collisions at ... TeV
(ProQuest: ... denotes formulae and/or non-USASCII text omitted; see image).A search for a light charged Higgs boson, originating from the decay of a top quark and subsequently decaying into a charm quark and a strange antiquark, is presented. The data used in the analysis correspond to an integrated luminosity of 19.7 fb super(-1) recorded in proton-proton collisions at ... TeV by the CMS experiment at the LHC. The search is performed in the process ..., where the W boson decays to a lepton (electron or muon) and a neutrino. The decays lead to a final state comprising an isolated lepton, at least four jets and large missing transverse energy. No significant deviation is observed in the data with respect to the standard model predictions, and model-independent upper limits are set on the branching fraction ..., ranging from 1.2 to 6.5% for a charged Higgs boson with mass between 90 and 160 GeV, under the assumption that ... [Figure not available: see fulltext.]
Measurement of electroweak production of a $$\\mathrm{W} $$ W boson in association with two jets in proton–proton collisions at $$\\sqrt{s}=13\\,\\text {Te}\\text {V} $$ s=13Te
A measurement is presented of electroweak (EW) production of a $$\\mathrm{W} $$ W boson in association with two jets in proton–proton collisions at $$\\sqrt{s}=13\\,\\text {Te}\\text {V} $$ s=13Te. The data sample was recorded by the CMS Collaboration at the LHC and corresponds to an integrated luminosity of 35.9 $$\\,\\text {fb}^{-1}$$ fb-1. The measurement is performed for the $$\\ell \\nu $$ ℓνjj final state (with $$\\ell \\nu $$ ℓν indicating a lepton–neutrino pair, and j representing the quarks produced in the hard interaction) in a kinematic region defined by invariant mass $$m_\\mathrm {jj} >120\\,\\text {Ge}\\text {V} $$ mjj>120Ge and transverse momenta $$p_\\mathrm {T j} > 25\\,\\text {Ge}\\text {V} $$ pTj>25Ge. The cross section of the process is measured in the electron and muon channels yielding $$\\sigma _\\mathrm {EW}(\\mathrm{W} \\mathrm {jj})= 6.23 \\pm 0.12 \\,\\text {(stat)} \\pm 0.61 \\,\\text {(syst)} \\,\\text {pb} $$ σEW(Wjj)=6.23±0.12(stat)±0.61(syst)pb per channel, in agreement with leading-order standard model predictions. The additional hadronic activity of events in a signal-enriched region is studied, and the measurements are compared with predictions. The final state is also used to perform a search for anomalous trilinear gauge couplings. Limits on anomalous trilinear gauge couplings associated with dimension-six operators are given in the framework of an effective field theory. The corresponding 95% confidence level intervals are $$-2.3< c_{{\\mathrm{W} \\mathrm{W} \\mathrm{W}}}/\\varLambda ^2 < 2.5\\,\\text {Te}\\text {V} ^{-2}$$ -2.3
Erratum to: Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at s = 13$$ \\sqrt{s}=13 $$TeV
In both panels of figure 11, the unit of the z axis was mistakenly written as “pb” when it should have been “fb”. The corrected versions are shown in figure 1.
Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at s = 13 $$ \\sqrt{s}=13 $$ TeV
Abstract A search for new physics is carried out in events with at least three electrons or muons in any combination, jets, and missing transverse momentum. Results are based on the sample of proton-proton collision data produced by the LHC at a center-of-mass energy of 13 TeV and collected by the CMS experiment in 2016. The data sample analyzed corresponds to an integrated luminosity of 35.9 fb−1. Events are classified according to the number of b jets, missing transverse momentum, hadronic transverse momentum, and the invariant mass of same-flavor dilepton pairs with opposite charge. No significant excess above the expected standard model background is observed. Exclusion limits at 95% confidence level are computed for four different supersymmetric simplified models with pair production of gluinos or third-generation squarks. In the model with gluino pair production, with subsequent decays into a top quark-antiquark pair and a neutralino, gluinos with masses smaller than 1610 GeV are excluded for a massless lightest supersymmetric particle. In the case of bottom squark pair production, the bottom squark masses are excluded up to 840 GeV for charginos lighter than 200 GeV. For a simplified model of heavy top squark pair production, the t˜2 $$ {\\tilde{\\mathrm{t}}}_2 $$ mass is excluded up to 720, 780, or 710 GeV for models with an exclusive t˜2→t˜1H $$ {\\tilde{\\mathrm{t}}}_2\\to {\\tilde{\\mathrm{t}}}_1\\mathrm{H} $$ decay, an exclusive t˜2→t˜1Z $$ {\\tilde{\\mathrm{t}}}_2\\to {\\tilde{\\mathrm{t}}}_1\\mathrm{Z} $$ decay, or an equally probable mix of those two decays. In order to provide a simplified version of the analysis for easier interpretation, a small set of aggregate signal regions also has been defined, providing a compromise between simplicity and analysis sensitivity.
Constraints on the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at s = 8$$ \\sqrt{s}=8 $$TeV
Abstract A first search for same-sign WW production via double-parton scattering is performed based on proton-proton collision data at a center-of-mass energy of 8 TeV using dimuon and electron-muon final states. The search is based on the analysis of data corresponding to an integrated luminosity of 19.7 fb−1. No significant excess of events is observed above the expected single-parton scattering yields. A 95% confidence level upper limit of 0.32 pb is set on the inclusive cross section for same-sign WW production via the double-parton scattering process. This upper limit is used to place a 95% confidence level lower limit of 12.2 mb on the effective double-parton cross section parameter, closely related to the transverse distribution of partons in the proton. This limit on the effective cross section is consistent with previous measurements as well as with Monte Carlo event generator predictions.
Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at s = 13$$ \\sqrt{s}=13 $$TeV
Abstract A search for narrow vector resonances decaying into quark-antiquark pairs is presented. The analysis is based on data collected in proton-proton collisions at s=13 $$ \\sqrt{s}=13 $$ TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb−1. The hypothetical resonance is produced with sufficiently high transverse momentum that its decay products are merged into a single jet with two-prong substructure. A signal would be identified as a peak over a smoothly falling background in the distribution of the invariant mass of the jet, using novel jet substructure techniques. No evidence for such a resonance is observed within the mass range of 50-300 GeV. Upper limits at 95% confidence level are set on the production cross section, and presented in a mass-coupling parameter space. The limits further constrain simplified models of dark matter production involving a mediator interacting between quarks and dark matter particles through a vector or axial-vector current. In the framework of these models, the results are the most sensitive to date, extending for the first time the search region to masses below 100 GeV.