# Large Strangeness as a QGP Signal in an Isentropic Quark-Hadron Phase Transition

Source: [Large Strangeness as a QGP Signal in an Isentropic Quark-Hadron Phase Transition](<https://www.sota2.com/research/paper/68fa1f2d7a2b558e29327aec>)

Collection index: [llms.txt](<https://www.sota2.com/research/llms.txt>)

Data updated: 2025-10-23T17:30:53.329Z

Authors: B. K. Patra, K. K. Singh, C. P. Singh

Published: 1998-09-11T05:47:54.000Z

## Abstract

Lattice QCD results reveal that the critical parameters and the order of the quark-hadron phase transition are quite sensitive to the number of dynamical flavours and their masses included in the theory. Motivated by this result we develop a phenomenological equation of state for the quark-gluon plasma consisting of $n\_f$ flavours retaining the entropy per baryon ratio continuous across the quark-hadron phase boundary. We thus obtain a generalised expression for the temperature and baryon chemical potential dependent bag constant. The results are shown for the realistic case, i.e., involving u, d and s quarks only. We then obtain a phase boundary for an isentropic quark-hadron phase transition using Gibbs' criteria. Similarly another phase boundary is obtained for the transition to an ideal QGP from the solution of the condition $B(\\mu,T)=0$. The variation of critical temperature $T\_c$ with the number of flavours included in the theory. Also the variation of ${(\\epsilon-4P)}/T^4$ with temperature are studied and compared with lattice results. Finally the strange particle ratios $\\frac{\\bar{\\Lambda}}{\\Lambda}$, $\\frac{\\bar{\\Xi}}{\\Xi}$ and $\\frac{K^+}{K^-}$ are obtained at both phase boundaries. We propose that their variations with the temperature and baryon chemical potential can be used in identifying the quark-gluon plasma in the recent as well as in future heavy-ion experiments.

## Recorded benchmark results

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## Original sources and implementation

[Original paper](<https://arxiv.org/abs/hep-ph/9809332>)

[PDF](<https://arxiv.org/pdf/hep-ph/9809332.pdf>)
