3 research outputs found

    Observation of nuclear modifications in W± boson production in pPb collisions at sNN=8.16TeV

    No full text
    The production of W± bosons is studied in proton-lead (pPb) collisions at a nucleon-nucleon centre-of-mass energy of sNN=8.16TeV. Measurements are performed in the W±→Ό±ΜΌ channel using a data sample corresponding to an integrated luminosity of 173.4±6.1nb−1, collected by the CMS Collaboration at the LHC. The number of positively and negatively charged W bosons is determined separately in the muon pseudorapidity region in the laboratory frame |ηlabÎŒ|25GeV/c. The W± boson differential cross sections, muon charge asymmetry, and the ratios of W± boson yields for the proton-going over the Pb-going beam directions are reported as a function of the muon pseudorapidity in the nucleon-nucleon centre-of-mass frame. The measurements are compared to the predictions from theoretical calculations based on parton distribution functions (PDFs) at next-to-leading-order. The results favour PDF calculations that include nuclear modifications and provide constraints on the nuclear PDF global fits

    Measurement of ttˉ\hbox {t}{\bar{\hbox {t}}} normalised multi-differential cross sections in pp{\text {p}}{\text {p}} collisions at s=13 TeV\sqrt{s}=13\,{\text {TeV}} , and simultaneous determination of the strong coupling strength, top quark pole mass, and parton distribution functions

    No full text
    Normalised multi-differential cross sections for top quark pair (ttˉ\hbox {t}{\bar{\hbox {t}}}) production are measured in proton-proton collisions at a centre-of-mass energy of 13 TeV\,{\text {TeV}} using events containing two oppositely charged leptons. The analysed data were recorded with the CMS detector in 2016 and correspond to an integrated luminosity of 35.9 fb−135.9{\,{\text {fb}}^{-1}} . The double-differential ttˉ\hbox {t}{\bar{\hbox {t}}} cross section is measured as a function of the kinematic properties of the top quark and of the ttˉ\hbox {t}{\bar{\hbox {t}}} system at parton level in the full phase space. A triple-differential measurement is performed as a function of the invariant mass and rapidity of the ttˉ\hbox {t}{\bar{\hbox {t}}} system and the multiplicity of additional jets at particle level. The data are compared to predictions of Monte Carlo event generators that complement next-to-leading-order (NLO) quantum chromodynamics (QCD) calculations with parton showers. Together with a fixed-order NLO QCD calculation, the triple-differential measurement is used to extract values of the strong coupling strength αS\alpha _{S} and the top quark pole mass (mtpolem_{{\text {t}}}^{{\text {pole}}}) using several sets of parton distribution functions (PDFs). The measurement of mtpolem_{{\text {t}}}^{{\text {pole}}} exploits the sensitivity of the ttˉ\hbox {t}{\bar{\hbox {t}}} invariant mass distribution to mtpolem_{{\text {t}}}^{{\text {pole}}} near the production threshold. Furthermore, a simultaneous fit of the PDFs, αS\alpha _{S}, and mtpolem_{{\text {t}}}^{{\text {pole}}} is performed at NLO, demonstrating that the new data have significant impact on the gluon PDF, and at the same time allow an accurate determination of αS\alpha _{S} and mtpolem_{{\text {t}}}^{{\text {pole}}}. The values αS(mZ)=0.1135−0.0017+0.0021\alpha _{S}(m_{{\text {Z}}}) = 0.1135{}^{+0.0021}_{-0.0017} and mtpole=170.5±0.8 GeVm_{{\text {t}}}^{{\text {pole}}} = 170.5 \pm 0.8 \,{\text {GeV}} are extracted, which account for experimental and theoretical uncertainties, the latter being estimated from NLO scale variations. Possible effects from Coulomb and soft-gluon resummation near the ttˉ\hbox {t}{\bar{\hbox {t}}} production threshold are neglected in these parameter extractions. A rough estimate of these effects indicates an expected correction of mtpolem_{{\text {t}}}^{{\text {pole}}} of the order of +1 GeV+1 \,{\text {GeV}} , which can be regarded as additional theoretical uncertainty in the current mtpolem_{{\text {t}}}^{{\text {pole}}} extraction

    Search for single production of vector-like quarks decaying to a top quark and a W boson in proton–proton collisions at s=13TeV

    Get PDF
    A search is presented for the single production of vector-like quarks in proton-proton collisions at s = 13 TeV . The data, corresponding to an integrated luminosity of 35.9 fb - 1 , were recorded with the CMS experiment at the LHC. The analysis focuses on the vector-like quark decay into a top quark and a W boson, with one muon or electron in the final state. The mass of the vector-like quark candidate is reconstructed from hadronic jets, the lepton, and the missing transverse momentum. Methods for the identification of b quarks and of highly Lorentz boosted hadronically decaying top quarks and W bosons are exploited in this search. No significant deviation from the standard model background expectation is observed. Exclusion limits at 95% confidence level are set on the product of the production cross section and branching fraction as a function of the vector-like quark mass, which range from 0.3 to 0.03 pb for vector-like quark masses of 700 to 2000 GeV . Mass exclusion limits up to 1660 GeV are obtained, depending on the vector-like quark type, coupling, and decay width. These represent the most stringent exclusion limits for the single production of vector-like quarks in this channel
    corecore