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Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV
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abstract
Measurements of identified hadrons as a function of the charged-particle multiplicity in pp collisions enable a search for the onset of collective effects in small collision systems. With such measurements, it is possible to study the mechanisms that determine the shapes of hadron transverse momentum ($p_{\rm{T}}$) spectra, to search for possible modifications of the yields of short-lived hadronic resonances due to scattering effects in the hadron-gas phase, and to investigate different explanations for the multiplicity evolution of strangeness production provided by phenomenological models. In this paper, these topics are addressed through measurements of the $\rm{K}^{*}(892)^{0}$ and $\phi(1020)$ mesons at midrapidity in pp collisions at $\sqrt{s}$ = 13 TeV as a function of the charged-particle multiplicity. The results include the $p_{\rm{T}}$ spectra, $p_{\rm{T}}$-integrated yields, mean transverse momenta, and the ratios of the yields of these resonances to those of longer-lived hadrons. Comparisons with results from other collision systems and energies, as well as predictions from phenomenological models, are also discussed.
Forward citations
Cited by 3 Pith papers
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Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV
First multiplicity-dependent measurement of charged K*(892) production in pp collisions at 13 TeV shows a 7-sigma suppression of the K*/K_S ratio from low to high multiplicity, mainly at low transverse momentum.
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Investigation of hadronic effects on resonance productions in small collision systems using the EPOS4 model
In EPOS4, resonance yields and mean transverse momenta are governed by a species-dependent balance between hadronic rescattering and regeneration even in pp, p-O, and O-O collisions.
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Examining hadronic resonance dynamics at energies available at the CERN Large Hadron Collider: Insights from EPOS4
EPOS4 with a hadronic afterburner reproduces resonance suppression patterns, and the extracted hadronic phase lifetime increases with multiplicity and system size, remaining non-zero in high-multiplicity pp collisions.
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