Yield ratio of hypertriton to light nuclei in heavy-ion collisions from = 4.9 GeV to 2.76 TeV
arXiv:2004.02385 · doi:10.1088/1674-1137/abadf0
Abstract
We resolve the difference in the yield ratio = measured in Au+Au collisions at = 200 GeV and in Pb-Pb collisions at = 2.76 TeV by adopting a different treatment of the weak decay contribution to the proton yield in Au+Au collisions at = 200 GeV. We then use the coalescence model to extract information on the and nucleon density fluctuations at the kinetic freeze-out of heavy ion collisions. We also show from available experimental data that the yield ratio = is a more promising observable than for probing the local baryon-strangeness correlation in the produced medium.
15 pages, 2 figures, 3 tables, submitted for publication
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Cited by in corpus (8)
- Properties of the QCD Matter -- An Experimental Review of Selected Results from RHIC BES Program
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- Coalescence, the thermal model and multi-fragmentation: The energy and volume dependence of light nuclei production in heavy ion collisions
- Observation of Directed Flow of Hypernuclei H and H in = 3 GeV Au+Au Collisions at RHIC
- Measurement of and binding energy in Au+Au collisions at = 3 GeV
- The effect of hadronic scatterings on the measurement of vector meson spin alignments in heavy-ion collisions
- Examination of background effects on light-nuclei yield ratio in relativistic heavy-ion collisions
- Production characteristics of light nuclei, hypertritons and -hypernuclei in Pb+Pb collisions at TeV