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Prompt D0, D+, and D+ production in Pb–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 5.02 TeV
The production of prompt D 0 , D + , and D *+ mesons was measured at midrapidity (| y | < 0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair $$ \sqrt{s_{\mathrm{NN}}} $$ s NN = 5 . 02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their had...
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Published in: | The journal of high energy physics 2022-01, Vol.2022 (1), Article 174 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The production of prompt D
0
, D
+
, and D
*+
mesons was measured at midrapidity (|
y
|
<
0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair
$$ \sqrt{s_{\mathrm{NN}}} $$
s
NN
= 5
.
02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0–10%) and semicentral (30–50%) collisions. The measurement was performed up to a transverse momentum (
p
T
) of 36 or 50 GeV/c depending on the D meson species and the centrality interval. For the first time in Pb–Pb collisions at the LHC, the yield of D
0
mesons was measured down to
p
T
= 0, which allowed a model-independent determination of the
p
T
-integrated yield per unit of rapidity (d
N/
d
y
). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor (
R
AA
) of prompt D mesons at
p
T
= 6–8 GeV/c for the 0–10% and 30–50% centrality classes, respectively. The D-meson
R
AA is compared with that of charged pions, charged hadrons, and J
/ψ
mesons as well as with theoretical predictions. The analysis of the agreement between the measured
R
AA
, elliptic (
v
2
) and triangular (
v
3
) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient
D
s
. Furthermore the comparison of
R
AA
and
v
2
with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP01(2022)174 |