[PDF] Top 20 Production of muons from heavy-flavour hadron decays in pp collisions at root s=5.02 TeV
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Production of muons from heavy-flavour hadron decays in pp collisions at root s=5.02 TeV
... Institute of Science and Technology Information and National Research Foundation of Korea (NRF), Republic of Korea; Ministry of Education and Scientific Research, Insti- tute of Atomic ... See full document
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D-meson Production In P-pb Collisions At Root S-nn=5.02 Tev And In Pp Collisions At Root S=7 Tev
... p-Pb collisions, minimum-bias events were selected, requiring at least one hit in both the V0A and the V0C scintillator ...arrays. In pp collisions, minimum-bias events were ... See full document
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Lambda(+)(c) production in pp collisions at root s=7 TeV and in p-Pb collisions at root s(NN)=5.02 TeV
... intepretation of the results in nucleus-nucleus collisions, the measurement in proton-nucleus collisions is also ...crucial. In such a system cold-nuclear-matter (CNM) ef- fects ... See full document
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Measurement of electrons from beauty-hadron decays in p-Pb collisions at root(NN)-N-S=5.02 TeV and Pb-Pb collisions at. root(NN)-N-S=2.76 TeV
... electrons from beauty-hadron decays, from charm-hadron decays, from photon conversions and electrons from other processes, which will be referred to as ‘Dalitz ... See full document
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Searches for light- and heavy-flavour three-jet resonances in pp collisions at root s=8 TeV
... a hadron calorimeter (HCAL) that consists of brass layers and scintillator sampling ...calorimeters. Muons are measured in gas ionisation detectors embedded in the steel return yoke ... See full document
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Measurement of electrons from open heavy-flavor hadron decays in pp at s = 13 TeV and electrons from beauty-hadron decays in Pb-Pb at sNN = 5.02 TeV collisions by ALICE at LHC
... 0.8). In this analysis, the non heavy-flavor electron background is identified via the data-driven photonic tagging method, leading to a high precision heavy-flavor electron cross ...prediction ... See full document
206
Searches for light- and heavy-flavour three-jet resonances in pp collisions at $\sqrt{s} = 8$ TeV
... results of dedicated searches for pair-produced three-jet resonances in multijet events from pp collisions, with one search being inclusive with respect to parton flavours and the ... See full document
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Measurement of the groomed jet mass in PbPb and pp collisions at root s(NN)=5:02 TeV
... feature of the CMS apparatus is a superconducting solenoid of 6 m internal di- ameter, providing an axial magnetic field of ...scintillator hadron calorimeter, each composed of a barrel ... See full document
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Inclusive J/psi production at mid-rapidity in pp collisions at root s=5.02 TeV
... mass of the bound state itself. In the CSM model, the pre-resonant cc state is assumed to be directly produced colourless and with the same quantum numbers as the final-state ...set of universal ... See full document
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Measurement of D0, D+, D*+ and Ds+ production in Pb-Pb collisions at root s(NN)=5:02 TeV
... and from 6% to 12% for the three-body decays of D + , D ∗+ and D + s ...+ s meson, the lower signal yield and the larger combinatorial background prevented a signal estimation without ... See full document
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Measurement of prompt J/psi pair production in pp collisions at root s = 7 Tev
... constructed from single-muon ...samples in data and simulation that contain sin- gle J/ψ decays to ...mesons in the event are neglected. The difference in the signal yield in ... See full document
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Search For Lepton Flavour Violating Decays Of Heavy Resonances And Quantum Black Holes To An E Mu Pair In Proton-proton Collisions At Root S=8 Tev
... impact of additional pp interactions in the same bunch crossing (pileup) on the selection efficiency, the calorimeter isolation is corrected for the average energy density in the event ... See full document
26
Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS
... scenarios of physics beyond the standard model predict the production at the Large Hadron Collider (LHC) of heavy particles with lifetimes that may be of order picoseconds ... See full document
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Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV
... distance from the primary vertex to the point of closest approach between the track and the jet axis, to be less than 5 ...contribution from tracks originating from pileup vertices is ... See full document
116
Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at root s=8 TeV
... presented in this paper, the signal signature contains a Z boson and a top quark, which both decay leptonically to either electrons or ...consists of three leptons (electrons and/or muons, including ... See full document
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Dielectron production in proton-proton collisions at root s=7 TeV
... ± s mesons (cτ ≈ ...have at least 100 out of a maximum of 159 reconstructed space points in the TPC with at least 100 crossed pad-rows, while the ITS track segments must have a ... See full document
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Strange particle production in pp collisions at root s=0.9 and 7 TeV
... vestigation of strange hadron production is an important ingredient in understanding the nature of the strong ...strange hadron production at √ s = 0.9 ... See full document
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Multiplicity dependence of light-flavor hadron production in pp collisions at root s=7 TeV
... γ S = 1, and the chemical potentials associated to baryon and electric charge quantum numbers are set to ...varied from 146 to 166 MeV as in ...results from lattice QCD calculations and their ... See full document
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Production of muons from heavy-flavour hadron decays in p-Pb collisions at root s(NN)=5.02 TeV
... V. Grigoriev 76 , A. Grigoryan 1 , S. Grigoryan 67 , N. Grion 112 , J.M. Gronefeld 100 , F. Grosa 30 , J.F. Grosse-Oetringhaus 34 , R. Grosso 100 , L. Gruber 115 , F.R. Grull 59 , F. Guber 52 , R. Guernane 72 , B. ... See full document
15
Elliptic Flow Of Electrons From Heavy-flavour Hadron Decays At Mid-rapidity In Pb-pb Collisions At Root S(nn)=2.76 Tev
... contributions of direct photons, thermal photons from the hot partonic and hadronic phase and photons that could be produced in the interactions of hard scattered partons with the medium, are ... See full document
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