2018-07-21
11:09 |
Detaljnije - Slični zapisi
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2018-07-21
11:09 |
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Non-strange and strange D-meson and charm-baryon production in heavy-ion collisions measured with ALICE at the LHC
/ Peng, Xinye
We present recent result on strange and non-strange D-meson production measured with ALICE in Pb--Pb collisions at the LHC. [...]
arXiv:1807.07286.
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00009 The $\Lambda_{{\rm c}}^+/{\rm D^0}$ ratio in Pb--Pb collisions at $\sqrt{s_{\scriptscriptstyle \rm NN}}$ = 5.02 TeV, compared with that in pp and p--Pb collisions (left), and $\Lambda_{{\rm c}}^+$-baryon $R_{\rm AA}$ in 0-80\% Pb--Pb collisions at 5.02 TeV compared to average non-strange D-meson, ${\rm D}_{\rm s}^+$-meson, $\pi ^\pm$ and charged particle $R_{\rm AA}$ in 0-10\% centrality class - 00007 The $\Lambda_{{\rm c}}/{\rm D^0}$ raito in pp collisions at $\sqrt{s}$ = 7 TeV and in p--Pb collisions at $\sqrt{s_{\scriptscriptstyle \rm NN}}$ = 5.02 TeV, compared with model predictions (left) and $\Lambda/{\rm K}^0_{\rm s}$, ${\rm p}/{\pi}$ ratios in pp (middle) and p--Pb (right) collisions. - 00006 Non-strange D-meson $R_{\rm AA}$ in the 0-10\% centrality class (left) and elliptic flow $v_{2}$ in the 30-50\% centrality class~\cite{v2} (right), compared with models predictions~\cite{LBT,MCsHQ,PHSD,POWLANG,Uphoff:2014hza,He:2014cla}. - 00011 Non-strange D-meson $R_{\rm AA}$ in the 0-10\% centrality class (left) and elliptic flow $v_{2}$ in the 30-50\% centrality class~\cite{v2} (right), compared with models predictions~\cite{LBT,MCsHQ,PHSD,POWLANG,Uphoff:2014hza,He:2014cla}. - 00008 The $\Lambda_{{\rm c}}^+/{\rm D^0}$ ratio in Pb--Pb collisions at $\sqrt{s_{\scriptscriptstyle \rm NN}}$ = 5.02 TeV, compared with that in pp and p--Pb collisions (left), and $\Lambda_{{\rm c}}^+$-baryon $R_{\rm AA}$ in 0-80\% Pb--Pb collisions at 5.02 TeV compared to average non-strange D-meson, ${\rm D}_{\rm s}^+$-meson, $\pi ^\pm$ and charged particle $R_{\rm AA}$ in 0-10\% centrality class - Fulltext - 00010 The $\Lambda_{{\rm c}}/{\rm D^0}$ raito in pp collisions at $\sqrt{s}$ = 7 TeV and in p--Pb collisions at $\sqrt{s_{\scriptscriptstyle \rm NN}}$ = 5.02 TeV, compared with model predictions (left) and $\Lambda/{\rm K}^0_{\rm s}$, ${\rm p}/{\pi}$ ratios in pp (middle) and p--Pb (right) collisions. - Fulltext
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Detaljnije - Slični zapisi
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2018-07-21
11:09 |
Detaljnije - Slični zapisi
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2018-07-20
18:21 |
Detaljnije - Slični zapisi
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2018-07-20
04:10 |
Detaljnije - Slični zapisi
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2018-07-20
04:10 |
Detaljnije - Slični zapisi
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2018-07-20
04:10 |
Detaljnije - Slični zapisi
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2018-07-20
04:10 |
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Heavy-flavour hadron decay leptons in Pb--Pb and Xe--Xe collisions at the LHC with ALICE
/ Dubla, Andrea
Heavy quarks, i.e. [...]
arXiv:1807.05382.
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Full text - 00009 Left: Comparison of the $R_{\rm AA}$ of electrons from beauty-hadron decays (red markers) with the one from charm- plus beauty-hadron decays (black markers) in Pb--Pb collisions at $\sqrt{s}$ = 5.02 TeV. Right: $R_{\rm AA}$ of electrons from beauty hadron decay in comparison with models implementing mass-dependent energy loss \cite{EPOS, Djordjevic, PHSD} in Pb--Pb collisions at $\sqrt{s}$ = 5.02 TeV. - 00010 Left: $R_{\rm AA}$ of electrons from heavy-flavour hadron decays as a function of $p_{\rm T}$ in central (0-10\%) Pb--Pb (black and grey markers) and in p--Pb (blue markers) collisions \cite{rpPbelectron} at $\sqrt{s}$ = 5.02 TeV. Right: $R_{\rm AA}$ of electrons from heavy-flavour hadron decays at $\sqrt{s}$ = 2.76 TeV in comparison with model calculations with and without the inclusion of the EPS09 shadowing parameterisations \cite{POWLANG, EPOS, TAMU}. - 00007 Nuclear modification factors of electrons (black markers) and muons (red markers) from heavy-flavour hadron decay in central (left panel) and semi-central (right panel) Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV. - 00006 Left: Comparison of the $R_{\rm AA}$ of electrons from beauty-hadron decays (red markers) with the one from charm- plus beauty-hadron decays (black markers) in Pb--Pb collisions at $\sqrt{s}$ = 5.02 TeV. Right: $R_{\rm AA}$ of electrons from beauty hadron decay in comparison with models implementing mass-dependent energy loss \cite{EPOS, Djordjevic, PHSD} in Pb--Pb collisions at $\sqrt{s}$ = 5.02 TeV. - 00008 $p_\mathrm{T}$-differential production cross section for electrons from heavy-flavour hadron decay in pp collisions at several collision energies (from left to right panel: $\sqrt{s}$ = 2.76, 5.02, 7 and 13 TeV) in comparison with FONLL calculations \cite{FONLL}. - 00011 Left: $R_{\rm AA}$ of electrons from heavy-flavour hadron decays as a function of $p_{\rm T}$ in central (0-10\%) Pb--Pb (black and grey markers) and in p--Pb (blue markers) collisions \cite{rpPbelectron} at $\sqrt{s}$ = 5.02 TeV. Right: $R_{\rm AA}$ of electrons from heavy-flavour hadron decays at $\sqrt{s}$ = 2.76 TeV in comparison with model calculations with and without the inclusion of the EPS09 shadowing parameterisations \cite{POWLANG, EPOS, TAMU}. - Fulltext
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Detaljnije - Slični zapisi
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2018-07-20
04:10 |
Detaljnije - Slični zapisi
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2018-07-20
04:10 |
Detaljnije - Slični zapisi
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