001     348436
005     20250630143500.0
024 7 _ |a 10.17182/HEPDATA.140124
|2 doi
037 _ _ |a GSI-2024-00272
041 _ _ |a English
100 1 _ |a ALICE Collaboration
|0 P:(DE-HGF)0
|b 0
|e Corresponding author
245 _ _ |a Production of pions, kaons and protons as a function of the transverse event activity in pp collisions at $\sqrt{s}=13$ TeV
260 _ _ |c 2023
336 7 _ |a MISC
|2 BibTeX
336 7 _ |a Dataset
|b dataset
|m dataset
|0 PUB:(DE-HGF)32
|s 1705418489_3067155
|2 PUB:(DE-HGF)
336 7 _ |a Chart or Table
|0 26
|2 EndNote
336 7 _ |a Dataset
|2 DataCite
336 7 _ |a DATA_SET
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336 7 _ |a ResearchData
|2 DINI
500 _ _ |a Journal Article GSI record: GSI-2024-00271
520 _ _ |a 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.
536 _ _ |a 612 - Cosmic Matter in the Laboratory (POF4-612)
|0 G:(DE-HGF)POF4-612
|c POF4-612
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536 _ _ |a HGS-HIRe - HGS-HIRe for FAIR (HGS-HIRe)
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536 _ _ |a SUC-GSI-Heidelberg - Strategic university cooperation GSI-U Heidelberg (SUC-GSI-HE)
|0 G:(DE-Ds200)SUC-GSI-HE
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536 _ _ |a SUC-GSI-Frankfurt - Strategic university cooperation GSI-U Frankfurt/M (SUC-GSI-FR)
|0 G:(DE-Ds200)SUC-GSI-FR
|c SUC-GSI-FR
|x 3
536 _ _ |a SUC-GSI-Darmstadt - Strategic university cooperation GSI-TU Darmstadt (SUC-GSI-DA)
|0 G:(DE-Ds200)SUC-GSI-DA
|c SUC-GSI-DA
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588 _ _ |a Dataset connected to DataCite
693 _ _ |a LHC
|e LHC: ALICE
|1 EXP:(DE-588)4398783-7
|0 EXP:(DE-H253)LHC-Exp-ALICE-20150101
|5 EXP:(DE-H253)LHC-Exp-ALICE-20150101
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773 _ _ |a 10.17182/HEPDATA.140124
787 0 _ |a Acharya, Shreyasi et.al.
|d [Trieste] : SISSA, 2023
|i RelatedTo
|0 GSI-2024-00271
|r arXiv:2301.10120 ; CERN-EP-2022-286
|t Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at $ \sqrt{s} $ = 13 TeV
909 C O |o oai:repository.gsi.de:348436
|p VDB
913 1 _ |a DE-HGF
|b Forschungsbereich Materie
|l Matter and the Universe
|1 G:(DE-HGF)POF4-610
|0 G:(DE-HGF)POF4-612
|3 G:(DE-HGF)POF4
|2 G:(DE-HGF)POF4-600
|4 G:(DE-HGF)POF
|v Cosmic Matter in the Laboratory
|x 0
914 1 _ |y 2023
920 _ _ |l yes
920 1 _ |0 I:(DE-Ds200)ALI-20080822OR105
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920 1 _ |0 I:(DE-Ds200)DTL-20051214OR031
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920 1 _ |0 I:(DE-Ds200)CIT-20110310OR121
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920 1 _ |0 I:(DE-Ds200)EXM-20080818OR100
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920 1 _ |0 I:(DE-Ds200)Coll-CERN-ALICE
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|l Collaboration CERN: ALICE
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980 _ _ |a dataset
980 _ _ |a VDB
980 _ _ |a I:(DE-Ds200)ALI-20080822OR105
980 _ _ |a I:(DE-Ds200)DTL-20051214OR031
980 _ _ |a I:(DE-Ds200)CIT-20110310OR121
980 _ _ |a I:(DE-Ds200)EXM-20080818OR100
980 _ _ |a I:(DE-Ds200)Coll-CERN-ALICE
980 _ _ |a UNRESTRICTED


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