Measurement of prompt and nonprompt charmonium suppression in $$\text {PbPb}$$ collisions at 5.02$$\,\text {Te}\text {V}
Abstract The nuclear modification factors of $${\mathrm {J}/\psi }$$ J / ψ and $$\psi \text {(2S)}$$ ψ (2S) mesons are measured in $$\text {PbPb}$$ PbPb collisions at a centre-of-mass energy per nucleon pair of $$\sqrt{\smash [b]{s_{_{\text {NN}}} = 5.02\,\text {Te}\text {V} $$ s NN = 5.02 TeV . The...
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Published in | The European physical journal. C, Particles and fields Vol. 78; no. 6 |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
United States
Springer
01.06.2018
|
Subjects | |
Online Access | Get full text |
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Summary: | Abstract
The nuclear modification factors of
$${\mathrm {J}/\psi }$$
J
/
ψ
and
$$\psi \text {(2S)}$$
ψ
(2S)
mesons are measured in
$$\text {PbPb}$$
PbPb
collisions at a centre-of-mass energy per nucleon pair of
$$\sqrt{\smash [b]{s_{_{\text {NN}}} = 5.02\,\text {Te}\text {V} $$
s
NN
=
5.02
TeV
. The analysis is based on
$$\text {PbPb}$$
PbPb
and
$$\mathrm {p}\mathrm {p}$$
p
p
data samples collected by CMS at the LHC in 2015, corresponding to integrated luminosities of 464
$$\,\mu \mathrm {b}^{-1}$$
μ
b
-
1
and 28
$$\,\text {pb}^\text {-1}$$
pb
-1
, respectively. The measurements are performed in the dimuon rapidity range of
$$|y | < 2.4$$
|
y
|
<
2.4
as a function of centrality, rapidity, and transverse momentum (
$$p_{\mathrm {T}}$$
p
T
) from
$$p_{\mathrm {T}} =3$$
p
T
=
3
$${\,\text {Ge}\text {V}/}\text {c}$$
GeV
/
c
in the most forward region and up to 50
$${\,\text {Ge}\text {V}/}\text {c}$$
GeV
/
c
. Both prompt and nonprompt (coming from b hadron decays)
$${\mathrm {J}/\psi }$$
J
/
ψ
mesons are observed to be increasingly suppressed with centrality, with a magnitude similar to the one observed at
$$\sqrt{\smash [b]{s_{_{\text {NN}}} = 2.76\,\text {Te}\text {V} $$
s
NN
=
2.76
TeV
for the two
$${\mathrm {J}/\psi }$$
J
/
ψ
meson components. No dependence on rapidity is observed for either prompt or nonprompt
$${\mathrm {J}/\psi }$$
J
/
ψ
mesons. An indication of a lower prompt
$${\mathrm {J}/\psi }$$
J
/
ψ
meson suppression at
$$p_{\mathrm {T}} > 25$$
p
T
>
25
$${\,\text {Ge}\text {V}/}\text {c}$$
GeV
/
c
is seen with respect to that observed at intermediate
$$p_{\mathrm {T}}$$
p
T
. The prompt
$$\psi \text {(2S)}$$
ψ
(2S)
meson yield is found to be more suppressed than that of the prompt
$${\mathrm {J}/\psi }$$
J
/
ψ
mesons in the entire
$$p_{\mathrm {T}}$$
p
T
range. |
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Bibliography: | FERMILAB-PUB-17-616-CMS; CMS-HIN-16-025; CERN-EP-2017-308; arXiv:1712.08959 AC02-07CH11359 USDOE Office of Science (SC), High Energy Physics (HEP) |
ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-018-5950-6 |