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@ARTICLE{Acharya:364000,
author = {Acharya, Shreyasi and others},
title = {{M}ultiplicity-dependent jet modification from di-hadron
correlations in pp collisions at $ \sqrt{s} $ = 13 {T}e{V}},
journal = {Journal of high energy physics},
volume = {03},
number = {3},
issn = {1126-6708},
address = {Heidelberg},
publisher = {Springer},
reportid = {GSI-2026-00202, arXiv:2409.04501. CERN-EP-2024-229},
pages = {194},
year = {2025},
note = {This article is distributed under the terms of the Creative
Commons Attribution License (CC-BY 4.0). Article funded by
SCOAP3.},
abstract = {Short-range correlations between charged particles are
studied via two-particle angular correlations in pp
collisions at $ \sqrt{s} $ = 13 TeV. The correlation
functions are measured as a function of the relative
azimuthal angle $∆{φ}$ and the pseudorapidity separation
$∆η$ for pairs of primary charged particles within the
pseudorapidity interval $|η|$ < 0.9 and the
transverse-momentum range 1 < p$_{T}$< 8 GeV/c. Near-side
($|∆φ|$ < 1.3) peak widths are extracted from a
generalised Gaussian fitted over the correlations in full
pseudorapidity separation ($|∆η|$< 1.8), while the
per-trigger associated near-side yields are extracted for
the short-range correlations ($|∆η|$ < 1.3). Both are
evaluated as a function of charged-particle multiplicity
obtained by two different event activity estimators. The
width of the near-side peak decreases with increasing
multiplicity, and this trend is reproduced qualitatively by
the Monte Carlo event generators PYTHIA 8, AMPT, and EPOS.
However, the models overestimate the width in the low
transverse-momentum region (p$_{T}$< 3 GeV/c). The
per-trigger associated near-side yield increases with
increasing multiplicity. Although this trend is also
captured qualitatively by the considered event generators,
the yield is mostly overestimated by the models in the
considered kinematic range. The measurement of the shape and
yield of the short-range correlation peak can help us
understand the interplay between jet fragmentation and event
activity, quantify the narrowing trend of the near-side peak
as a function of transverse momentum and multiplicity
selections in pp collisions, and search for final-state jet
modification in small collision systems.},
keywords = {Hadron-Hadron Scattering (autogen) / Particle Correlations
and Fluctuations (autogen) / QCD (autogen)},
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) / STRONG-2020 - The strong
interaction at the frontier of knowledge: fundamental
research and applications (824093)},
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 / G:(EU-Grant)824093},
experiment = {EXP:(DE-H253)LHC-Exp-ALICE-20150101},
typ = {PUB:(DE-HGF)16},
eprint = {2409.04501},
howpublished = {arXiv:2409.04501},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2409.04501;\%\%$},
UT = {WOS:001489942100001},
doi = {10.1007/JHEP03(2025)194},
url = {https://repository.gsi.de/record/364000},
}