1,722,545 research outputs found

    Measurement of Differential ttˉ{\rm t}\bar{\rm t} Cross Sections at 7 TeV

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    A measurement is presented of the normalized differential cross sections of top-quark pair production in pp collisions at a center of mass energy of 7 TeV, using 1.1 fb1^{-1} of data collected in 2011 by the CMS experiment. The measurement is performed using five different final states with one or two muons or electrons in the final state. The event selections yield high purity ttˉ{\rm t}\bar{\rm t} samples. Kinematic reconstructions are performed to obtain full information of the top quarks, the ttˉ{\rm t}\bar{\rm t} system and the final state leptons. The results are compared to several QCD predictions up to next-to-leading order

    Studies of ttˉ\rm t\bar{t}+X at CMS

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    This talk is dedicated to the most recent measurements of the processes that feature the production of a top quark pair either with an electroweak standard model boson, or another pair of top, bottom or light quarks. For the measurement of the production cross-section of top quark pair in association with a photon, 19.7 fb1\rm fb^{-1} of proton-proton collision data collected by CMS detector at s\sqrt{s} = 8 TeV is used, while for four top production, ttˉ\rm t\bar{t} + bb, ttˉ\rm t\bar{t} + jj, ttˉ\rm t\bar{t}W and ttˉ\rm t\bar{t}Z the data collected at s\sqrt{s} = 13 TeV amounting to 35.9 fb1\rm fb^{-1}, is used. The measurement of ttˉγ\rm t\bar{t}\gamma is performed in the fiducial phase space corresponding to the semileptonic decay chain of the top quark pair, and the cross section is measured relative to the inclusive top quark pair production cross section. The fiducial cross section for this process is found to be 127 ±\pm 27 (stat + syst) fb. The most recent search for the four top quark production, that explores the same-sign dilepton final state, set the upper observed (expected) limit to 4.6 (2.90.9+1.42.9^{+1.4}_{-0.9}) times predicted standard model cross section. The measured cross section of the top pair production with two b quarks is found to be σ\sigma(ttˉ\rm t\bar{t} + bb) = 3.9 ±\pm 0.6 (stat) ±\pm 1.3 (syst) pb in the full phase space. The measurement of the ttˉ\rm t\bar{t}W and ttˉ\rm t\bar{t}Z processes combines three final states with two same-sign, three and four leptons. The ttˉ\rm t\bar{t}W and ttˉ\rm t\bar{t}Z production cross sections are measured to be σ\sigma(ttˉ\rm t\bar{t}Z) = 1.000.08+0.09(stat.)0.10+0.12(sys.)\rm 1.00^{+0.09}_{-0.08} (stat.)^{+0.12}_{-0.10} (sys.) pb and σ\sigma(ttˉ\rm t\bar{t}W) = 0.800.11+0.12(stat.)0.12+0.13(sys.)\rm 0.80^{+0.12}_{-0.11} (stat.)^{+0.13}_{-0.12} (sys.) pb with an expected (observed) significance of 4.6 (5.5) and 9.5 (9.9) standard deviations from the background-only hypothesis. The latter measurements are used to constrain the Wilson coefficients for four dimension-six operators describing interactions of new physics that would modify ttˉ\rm t\bar{t}W and ttˉ\rm t\bar{t}Z production

    Reflexió crítica sobre RM/T

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    S'analitza el nou model relacional RM/T d'En Codd, criticant-ne diferents punts, en particular els referents al paper de les "entitats", i situant-lo en relació a altres recerques

    Reflexió crítica sobre RM/T

    No full text
    S'analitza el nou model relacional RM/T d'En Codd, criticant-ne diferents punts, en particular els referents al paper de les "entitats", i situant-lo en relació a altres recerques.Postprint (published version

    Reflexió crítica sobre RM/T

    No full text
    S'analitza el nou model relacional RM/T d'En Codd, criticant-ne diferents punts, en particular els referents al paper de les "entitats", i situant-lo en relació a altres recerques.Postprint (published version

    Measurements of ttˉ+jets{\rm t\bar t+jets}, ttˉ+bbˉ{\rm t\bar t+b\bar b} production, and ttˉttˉ{\rm t\bar tt\bar t} production at CMS

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    The most recent CMS measurements of the production of ttˉ{\rm t\bar t} pairs with two additional jets, or two additional b quarks, are presented. These two processes are important for several reasons: they can allow a better modeling of Monte Carlo simulations, because of the different energy scale associated to b-jets and generic jets; they are important backgrounds to other standard model processes; and they might be related to new physics. In addition, the search for the production of two ttˉ{\rm t\bar t} pairs is discussed, along with its connection to the Yukawa coupling of top quarks to the Higgs boson

    B-meson hadroproduction in the SACOT-mTm_{\rm T} scheme

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    We apply the SACOT-mTm_{\rm T} general-mass variable flavour number scheme (GM-VFNS) to the inclusive B-meson production in hadronic collisions at next-to-leading order in perturbative Quantum Chromodynamics. In the GM-VFNS approach one matches the fixed-order heavy-quark production cross sections, accurate at low transverse momentum (pTp_{\rm T}), with the zero-mass cross sections, accurate at high pTp_{\rm T}. The physics idea of the SACOT-mTm_{\rm T} scheme is to do this by accounting for the finite momentum transfer required to create a heavy quark-antiquark pair throughout the calculation. We compare our results with the latest LHC data from proton-proton and proton-lead collisions finding a very good agreement within the estimated theoretical uncertainties. We discuss also scheme-related differences and their impact on the scale uncertainties.Comment: Version that matches with the one accepted for publicatio

    Energy dependence of light neutral meson pTp_{\rm T} spectrum produced in pp collisions at the LHC measured in ALICE

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    We present the measurement of light neutral mesons, π0\pi^{0} and η\eta, in pp collisions at different center-of-mass energies obtained with the ALICE experiment at the LHC. The π0\pi^{0} and η\eta mesons are measured via photons reconstructed by the electromagnetic calorimeters and the central tracking system. The invariant cross-section of π0\pi^{0} and η\eta mesons are measured in a broad pTp_{\rm T} range at s=0.9,2.76,7,5.02\sqrt{s} = 0.9, 2.76, 7, 5.02 and 8 TeV. The spectra of π0\pi^{0} and η\eta mesons measured in pp collisions at different collision energies show xTx_{\rm T}-scaling at high pTp_{\rm T} and violation of mTm_{\rm T}-scaling at low pTp_{\rm T}. The smaller xTx_{\rm T}-scaling exponents of our measurements compared to RHIC may hint at a reduced importance of higher twist processes at LHC

    Quantification of the low-pTp_{\rm T} pion excess in heavy-ion collisions at the LHC and top RHIC energy

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    A Bayesian inference analysis is performed to quantify the pion excess in the low transverse momentum (pTp_{\rm T}) regime in heavy-ion collisions. This quantification is conducted across centrality classes and collision systems at the LHC and top RHIC energy. The analysis is based on the relativistic fluid dynamics description of pTp_{\rm T} spectra of identified charged hadrons. A pTp_{\rm T} range scan investigation to determine the optimal range for the pion pTp_{\rm T} spectra with respect to a fluid dynamic description is performed, finding 0.5~<pT<< p_{\rm T} < ~2.0~GeV/c/c. A significant low-pTp_{\rm T} pion excess is computed across all centrality classes and collision systems investigated, indicating that a clear low-pTp_{\rm T} component arises from different physics mechanisms, rather than thermal production. Further comparison with measurements by the PHOBOS Collaboration confirms the persistence of the pion excess into very low-pTp_{\rm T}, with no enhancement observed in kaons and protons within the current experimental precision.Comment: 9 pages, 6 figure
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