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@ARTICLE{Acharya:250878,
author = {Acharya, Shreyasi and others},
title = {{C}harm-quark fragmentation fractions and production cross
section at midrapidity in pp collisions at the {LHC}},
journal = {Physical review / D},
volume = {105},
number = {1},
issn = {2470-0010},
address = {Melville, NY},
publisher = {Inst.},
reportid = {GSI-2023-00110, arXiv:2105.06335. CERN-EP-2021-088},
pages = {L011103},
year = {2022},
note = {ISSN 2470-0029 not unique: **3 hits**.Phys. Rev. D 105,
L011103 (2022). 20 pages, 2 captioned figures, 1 table,
authors from page 14, published version, figures at
https://alice-publications.web.cern.ch/node/7107SCOAP3
ccby4.0},
abstract = {Recent p$_T$-integrated cross-section measurements of the
ground-state charm mesons and baryons, D$^0$, D$^+$,
D$_s^+$, Λ$_c^+$, and Ξ$_c^0$, are used to evaluate the
charm fragmentation fractions and production cross section
per unit of rapidity at midrapidity (|y|<0.5), in pp
collisions at $\sqrt{s}$ = 5.02 TeV at the LHC. The latter
is dσ$_{c\bar{c}}$/dy|$_{|y|<0.5}$ = 1165 ± 44(stat) -101
+ 134(syst) μb. These measurements were obtained for the
first time in hadronic collisions at the LHC, including the
charm baryon states, recently measured by ALICE at
midrapidity. The charm fragmentation fractions differ
significantly from the values measured in e$^+$e$^-$ and ep
collisions, providing evidence of the dependence of the
parton-to-hadron fragmentation fractions on the collision
system, indicating that the assumption of their universality
is not supported by the measured cross sections. An increase
of a factor of about 3.3 for the fragmentation fraction for
the Λ$_c^+$ with a significance of 5σ between the values
obtained in pp collisions and those obtained in e$^+$e$^-$
(ep) collisions is reported. The fragmentation fraction for
the Ξ$_c^0$ was obtained for the first time in any
collision system. The measured fragmentation fractions were
used to update the $c\bar{c}$ cross sections per unit of
rapidity at |y| < 0.5 at $\sqrt{s}$ = 2.76 and 7 TeV, which
are about 40\% higher than the previously published results.
The data were compared with perturbative-QCD calculations
and lie at the upper edge of the theoretical bands.},
keywords = {charm: fragmentation (INSPIRE) / p p: scattering (INSPIRE)
/ electron p: interaction (INSPIRE) / charm: ground state
(INSPIRE) / quantum chromodynamics: perturbation theory
(INSPIRE) / cross section: measured (INSPIRE) / hadron
hadron: interaction (INSPIRE) / CERN LHC Coll (INSPIRE) /
rapidity (INSPIRE) / ALICE (INSPIRE) / experimental results
(INSPIRE) / 2760 GeV-cms/nucleon (INSPIRE) / 5020
GeV-cms/nucleon (INSPIRE) / 7000 GeV-cms/nucleon (INSPIRE)},
cin = {ALI / DTL / CIT / EXM / ALICE@CERN},
ddc = {530},
cid = {I:(DE-Ds200)ALI-20080822OR105 /
I:(DE-Ds200)DTL-20051214OR031 /
I:(DE-Ds200)CIT-20110310OR121 /
I:(DE-Ds200)EXM-20080818OR100 / I:(DE-Ds200)Coll-CERN-ALICE},
pnm = {612 - Cosmic Matter in the Laboratory (POF4-612) / HGS-HIRe
- HGS-HIRe for FAIR (HGS-HIRe) / SUC-GSI-Heidelberg -
Strategic university cooperation GSI-U Heidelberg
(SUC-GSI-HE) / SUC-GSI-Frankfurt - Strategic university
cooperation GSI-U Frankfurt/M (SUC-GSI-FR) /
SUC-GSI-Darmstadt - Strategic university cooperation GSI-TU
Darmstadt (SUC-GSI-DA)},
pid = {G:(DE-HGF)POF4-612 / G:(DE-Ds200)HGS-HIRe /
G:(DE-Ds200)SUC-GSI-HE / G:(DE-Ds200)SUC-GSI-FR /
G:(DE-Ds200)SUC-GSI-DA},
experiment = {EXP:(DE-H253)LHC-Exp-ALICE-20150101},
typ = {PUB:(DE-HGF)16},
eprint = {2105.06335},
howpublished = {arXiv:2105.06335},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2105.06335;\%\%$},
UT = {WOS:000748867800001},
doi = {10.1103/PhysRevD.105.L011103},
url = {https://repository.gsi.de/record/250878},
}