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[PDF] Top 20 Measurement Of Electrons From Heavy-flavour Hadron Decays In P-pb Collisions At Root S(nn)=5.02 Tev

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Measurement Of Electrons From Heavy-flavour Hadron Decays In P-pb Collisions At Root S(nn)=5.02 Tev

Measurement Of Electrons From Heavy-flavour Hadron Decays In P-pb Collisions At Root S(nn)=5.02 Tev

... tion of the experiment and the CERN accelerator teams for the out- standing performance of the LHC ...support in building and running the ALICE detector: State Committee of Science, World ... See full document

14

Azimuthal anisotropy of heavy-flavor decay electrons in p-Pb collisions at root s(NN)=5.02 TeV

Azimuthal anisotropy of heavy-flavor decay electrons in p-Pb collisions at root s(NN)=5.02 TeV

... construction of the experiment and the CERN accelerator teams for the outstanding performance of the LHC ...support in building and running the ALICE detector: the ...Committee of Science and ... See full document

14

Measurement of dijet k(T) in p-Pb collisions at root s(NN)=5.02 TeV

Measurement of dijet k(T) in p-Pb collisions at root s(NN)=5.02 TeV

... , of 15 GeV/c and is always of lower transverse momentum than the full ...tum of the full jet. Increasing the transverse momentum of the full jet extends the kinematic reach of | k Ty| ... See full document

12

Measurement of D0, D+, D*+ and Ds+ production in Pb-Pb collisions at root s(NN)=5:02 TeV

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

36

Measurement of dielectron production in central Pb-Pb collisions at root S-NN=2.76 TeV

Measurement of dielectron production in central Pb-Pb collisions at root S-NN=2.76 TeV

... originate from tracking, particle identification, pho- ton conversion rejection, hadron contamination and back- ground ...description of the detector and of real data by MC simulations that ... See full document

24

Elliptic Flow Of Muons From Heavy-flavour Hadron Decays At Forward Rapidity In Pb-pb Collisions At Root S(nn)=2.76tev

Elliptic Flow Of Muons From Heavy-flavour Hadron Decays At Forward Rapidity In Pb-pb Collisions At Root S(nn)=2.76tev

... tor of muons from heavy-flavour hadron decays [21] are com- pared to the following three ...propagation of heavy quarks in the medium including collisional and ... See full document

17

Measurements of low-pT electrons from semileptonic heavy-flavour hadron decays at mid-rapidity in pp and Pb-Pb collisions at root s(NN)=2.76 TeV

Measurements of low-pT electrons from semileptonic heavy-flavour hadron decays at mid-rapidity in pp and Pb-Pb collisions at root s(NN)=2.76 TeV

... a heavy-flavour enriched PYTHIA 6 [ 64 ] MC sample in which each simulated pp event contains a c¯ c or b¯ b pair, and heavy-flavour hadrons are forced to decay ...semi-electronically. ... See full document

31

Two-pion femtoscopy in p-Pb collisions at root(NN)-N-S=5.02 TeV

Two-pion femtoscopy in p-Pb collisions at root(NN)-N-S=5.02 TeV

... pp collisions ats = 0.9 and 7 TeV [ 15 – 18 ] and compared to results from heavy-ion collisions at lower collision ...(i) In A-A collisions all ... See full document

19

Measurement Of D-meson Production Versus Multiplicity In P-pb Collisions At Root S(nn)=5.02 Tev

Measurement Of D-meson Production Versus Multiplicity In P-pb Collisions At Root S(nn)=5.02 Tev

... methods in order to determine the systematic uncertainties related to the extraction of the raw D-meson ...widths of the histograms, and considering different functions to describe the background, ... See full document

45

Measurement of upsilon(1S) elliptic flow at forward rapidity in Pb-Pb collisions at root s(NN)=5.02 TeV

Measurement of upsilon(1S) elliptic flow at forward rapidity in Pb-Pb collisions at root s(NN)=5.02 TeV

... polynomial. In addition, the signal CB2 tail parameters and background fit functions are varied [35] ...choice of fitting ...increases from 0.004 to 0.016 with increasing collision centrality and ... See full document

14

Measurement of the B-+/- meson nuclear modification factor in Pb-Pb collisions at root s(NN)=5.02 TeV

Measurement of the B-+/- meson nuclear modification factor in Pb-Pb collisions at root s(NN)=5.02 TeV

... and of the energy loss sources (partonic only [45,47] or also hadronic [45] ), the set of the (nuclear) parton distribution functions used for the initial heavy-quark p T distributions, ... See full document

18

W And Z Boson Production In P-pb Collisions At Tev Root S(nn)=5.02 Tev

W And Z Boson Production In P-pb Collisions At Tev Root S(nn)=5.02 Tev

... section at backward rapidity is estimated from two reconstructed Z boson candidates (see left panel of figure 1 ...). In this case, the statistical uncertainty is defined as the 68% confidence ... See full document

28

D-meson Production In P-pb Collisions At Root S-nn=5.02 Tev And In Pp Collisions At Root S=7 Tev

D-meson Production In P-pb Collisions At Root S-nn=5.02 Tev And In Pp Collisions At Root S=7 Tev

... Background: In the context of the investigation of the quark gluon plasma produced in heavy-ion collisions, hadrons containing heavy (charm or beauty) quarks play a ... See full document

32

Lambda(+)(c) production in pp collisions at root s=7 TeV and in p-Pb collisions at root s(NN)=5.02 TeV

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- ... See full document

49

Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at root s(NN)=5.02 TeV

Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at root s(NN)=5.02 TeV

... applied in a theoretical calcu- lation at any stage of a parton shower and at final state particle ...class of algorithms in this con- text are those using sequential ... See full document

15

Production of muons from heavy-flavour hadron decays in p-Pb collisions at root s(NN)=5.02 TeV

Production of muons from heavy-flavour hadron decays in p-Pb collisions at root s(NN)=5.02 TeV

... Council of Norway, Norway; Commission on Science and Technology for Sus- tainable Development in the South (COMSATS), Pakistan; Pontificia Universidad Católica del Perú, Peru; Ministry of Science and ... 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

Elliptic Flow Of Electrons From Heavy-flavour Hadron Decays At Mid-rapidity In Pb-pb Collisions At Root S(nn)=2.76 Tev

... Council of Norway (NFR); Pontificia Universidad Cat´ olica del Per´ u; National Science Centre, Poland; Ministry of Na- tional Education/Institute for Atomic Physics and National Council of ... See full document

42

Measurement of the production of high-p(T) electrons from heavy-flavour hadron decays in Pb-Pb collisions at root s(NN)=2.76 TeV

Measurement of the production of high-p(T) electrons from heavy-flavour hadron decays in Pb-Pb collisions at root s(NN)=2.76 TeV

... Additional hadron rejection used the combination of the energy deposited within EMCal and a cut on the electromagnetic shower shape [64,66] ...shower from an electron is fully contained and ... See full document

16

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

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

... Ministry of Education, Research and Religious Affairs, Greece; National Research, Development and Innovation Office, Hungary; Department of Atomic Energy Government of India (DAE), India; Indonesian ... See full document

41

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

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

... description of their initial production (that can include cold nuclear matter effects or not), a description of the space-time evolution of the QGP up to the freeze-out, mechanisms of ... See full document

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