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Strange baryon resonance production in $\sqrt{s_{NN}} = 200$ GeV $p+p$ and $Au+Au$ collisions
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arxiv nucl-ex/0604019 v2 pith:SJSUNUI5 submitted 2006-04-27 nucl-ex
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abstract
We report the measurements of $\Sigma (1385)$ and $\Lambda (1520)$ production in $p+p$ and $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV from the STAR collaboration. The yields and the $p_{T}$ spectra are presented and discussed in terms of chemical and thermal freeze-out conditions and compared to model predictions. Thermal and microscopic models do not adequately describe the yields of all the resonances produced in central $Au+Au$ collisions. Our results indicate that there may be a time-span between chemical and thermal freeze-out during which elastic hadronic interactions occur.
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Cited by 3 Pith papers
Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. OpenAlex reports about 122 citations worldwide. Full citation record
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Observation of the centrality-dependent difference in directed flow between charged kaons and $K^{*0}$ resonances in Au+Au collisions at $\sqrt{s_{\mathrm{NN}}}$ = 14.6, 19.6 and 27 GeV
nucl-ex 2026-07 accept novelty 7.0 of 10
First measurement of K*0 directed flow shows a centrality-dependent difference from charged kaons that hydro+UrQMD models attribute to asymmetric hadronic rescattering relative to the event plane.
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Probing Late-Stage Hadronic Interactions at High Baryon Density via $K^{*0}$ Production in the RHIC Beam Energy Scan Program
nucl-ex 2026-01 accept novelty 7.0 of 10
K*0/K yield ratios in central Au+Au collisions at BES energies are suppressed relative to peripheral collisions and thermal predictions, indicating hadronic rescattering that strengthens at lower energies.
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Examining hadronic resonance dynamics at energies available at the CERN Large Hadron Collider: Insights from EPOS4
hep-ph 2024-12 conditional novelty 4.0 of 10
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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