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@ARTICLE{Acharya:250934,
author = {Acharya, Shreyasi and others},
title = {{O}bservation of a multiplicity dependence in the $p_{\rm
{T}}$-differential charm baryon-to-meson ratios in
proton-proton collisions at $\sqrt{s} = 13$ {T}e{V}},
journal = {Physics letters / B},
volume = {829},
issn = {0031-9163},
address = {Amsterdam},
publisher = {North-Holland Publ.},
reportid = {GSI-2023-00146, arXiv:2111.11948. CERN-EP-2021-245},
pages = {137065},
year = {2022},
note = {Phys.Lett.B 829 (2022) 137065. 25 pages, 5 captioned
figures, 1 table, authors from page 20, published version,
figures at
http://alice-publications.web.cern.ch/node/7524SCOAP3.
ccby4.0},
abstract = {The production of prompt D0, Ds+, and Λc+ hadrons, and
their ratios, Ds+/D0 and Λc+/D0, are measured in
proton–proton collisions at $\sqrt{s}$ = 13 TeV at
midrapidity (|y|<0.5) with the ALICE detector at the LHC.
The measurements are performed as a function of the
charm-hadron transverse momentum (p$_T$) in intervals of
charged-particle multiplicity, measured with two
multiplicity estimators covering different pseudorapidity
regions. While the strange to non-strange Ds+/D0 ratio
indicates no significant multiplicity dependence, the
baryon-to-meson p$_T$-differential Λc+/D0 ratio shows a
multiplicity-dependent enhancement, with a significance of
5.3σ for 1 < p$_T$ <12 GeV/c, comparing the highest
multiplicity interval with respect to the lowest one. The
measurements are compared with a theoretical model that
explains the multiplicity dependence by a canonical
treatment of quantum charges in the statistical
hadronisation approach, and with predictions from event
generators that implement colour reconnection mechanisms
beyond the leading colour approximation to model the
hadronisation process. The Λc+/D0 ratios as a function of
p$_T$ present a similar shape and magnitude as the Λ/KS0
ratios in comparable multiplicity intervals, suggesting a
potential common mechanism for light- and charm-hadron
formation, with analogous multiplicity dependence. The
p$_T$-integrated ratios, extrapolated down to p$_T$ = 0, do
not show a significant dependence on multiplicity within the
uncertainties.},
keywords = {multiplicity: dependence (INSPIRE) / p p: scattering
(INSPIRE) / hadronization: statistical (INSPIRE) / charged
particle: multiplicity (INSPIRE) / hadronization: model
(INSPIRE) / rapidity: difference (INSPIRE) / color (INSPIRE)
/ ALICE (INSPIRE) / transverse momentum (INSPIRE) / CERN LHC
Coll (INSPIRE) / charm (INSPIRE) / hadron (INSPIRE) / Monte
Carlo (INSPIRE) / experimental results (INSPIRE) / 13000
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 = {2111.11948},
howpublished = {arXiv:2111.11948},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2111.11948;\%\%$},
UT = {WOS:000821534900019},
doi = {10.1016/j.physletb.2022.137065},
url = {https://repository.gsi.de/record/250934},
}