% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@MISC{Collaboration:348436,
author = {{ALICE Collaboration}},
title = {{P}roduction of pions, kaons and protons as a function of
the transverse event activity in pp collisions at
$\sqrt{s}=13$ {T}e{V}},
reportid = {GSI-2024-00272},
year = {2023},
note = {Journal Article GSI record: GSI-2024-00271},
abstract = {The production of $\pi^{\pm}$, $\mathrm{K}^{\pm}$, and
$(\mathrm{\overline{p}})\mathrm{p}$ is measured in pp
collisions at $\sqrt{s}\,= 13~\mathrm{TeV}$ in different
topological regions of the events. Particle transverse
momentum $(p_{\mathrm{T}})$ spectra are measured in the
``toward'', ``transverse'', and ``away'' angular regions
defined with respect to the direction of the leading
particle in the event. While the toward and away regions
contain the fragmentation products of the near-side and
away-side jets, respectively, the transverse region is
dominated by particles from the Underlying Event (UE). The
relative transverse activity classifier, $R_{\mathrm{T}} =
N_{\mathrm{T}} / \langle N_{\mathrm{T}} \rangle$, is used to
group events according to their UE activity, where
$N_{\mathrm{T}}$ is the measured charged-particle
multiplicity per event in the transverse region and $\langle
N_{\mathrm{T}} \rangle$ is the mean value over all the
analysed events. The first measurements of identified
particle $p_{\mathrm{T}}$ spectra as a function of
$R_{\mathrm{T}}$ in the three topological regions are
reported. It is found that the yield of high transverse
momentum particles relative to the
$R_{\mathrm{T}}$-integrated measurement decreases with
increasing $R_{\mathrm{T}}$ in both the toward and the away
regions, indicating that the softer UE dominates particle
production as $R_{\mathrm{T}}$ increases and validating that
$R_{\mathrm{T}}$ can be used to control the magnitude of the
UE. Conversely, the spectral shapes in the transverse region
harden significantly with increasing $R_{\mathrm{T}}$. This
hardening follows a mass ordering, being more significant
for heavier particles. Finally, it is observed that the
$p_{\mathrm{T}}$-differential particle ratios $(\mathrm{p} +
\mathrm{\overline{p}})/(\pi^{+} + \pi^{-})$ and
$(\mathrm{K}^{+} + \mathrm{K}^{-})/(\pi^{+} + \pi^{-})$ in
the low UE limit $(R_{\mathrm{T}} \rightarrow 0)$ approach
expectations from Monte Carlo generators such as PYTHIA 8
and EPOS LHC, where the jet-fragmentation models have been
tuned to reproduce $\mathrm{e}^{+}\mathrm{e}^{-}$ results.},
cin = {ALI / DTL / CIT / EXM / ALICE@CERN},
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)32},
doi = {10.17182/HEPDATA.140124},
url = {https://repository.gsi.de/record/348436},
}