Proceedings of XIII Quark Confinement and the Hadron Spectrum — PoS(Confinement2018) 2019
DOI: 10.22323/1.336.0145
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Hadron gas with repulsive mean field

Abstract: We study the QCD equation of state, and fluctuations of baryon number and strangeness using the hadron resonance gas model with repulsive mean field. We find that including both the predicted but not observed resonances, a.k.a. missing states, and the repulsive mean field into the resonance gas model leads to better description of the lattice results. The repulsive mean field is particularly important for the higher order baryon number fluctuations.

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Cited by 4 publications
(10 citation statements)
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“…Within this approach one can estimate the difference between the second order fluctuations and correlations of conserved charges and the fourth and sixth order fluctuations and correlations. The model can explain these differences reasonably well [7] if one assumes that only ground state octet and decuplet baryons are affected by the repulsive interactions.…”
Section: Pos(cpod2017)034mentioning
confidence: 97%
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“…Within this approach one can estimate the difference between the second order fluctuations and correlations of conserved charges and the fourth and sixth order fluctuations and correlations. The model can explain these differences reasonably well [7] if one assumes that only ground state octet and decuplet baryons are affected by the repulsive interactions.…”
Section: Pos(cpod2017)034mentioning
confidence: 97%
“…the mean-field is repulsive. In what follows we will use the value K = 450 MeV/fm 3 , which is consistent withb 2 (T ) at the highest temperatures [7]. It is straightforward to generalize the mean-field approach described above to a multicomponent system, e.g.…”
Section: Pos(cpod2017)034mentioning
confidence: 99%
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