The role of finite value of strange quark mass (ms≠0) and baryon number density (n) on the stability and maximum mass of strange stars
Abstract
This study describes the impact of non-zero value of strange quark mass (ms) and number density of baryons (n) on the structure, stability and maximum mass of strange stars. We derive an exact relativistic solution of the Einstein field equation using the Tolman-IV metric potential and modified MIT bag model EoS, pr=13(-4B'), where B' is a function of bag constant B, ms and baryon number density (n). Following CERN's findings, transition of phase from hadronic matter to Quark-Gluon Plasma (QGP) may occur at high densities in presence of favourable conditions. The standard MIT bag model, with a constant B, fails to explain such transition properly. Introducing a finite ms and Wood-Saxon parametrisation for B, dependent on baryon number density (n), provides a more realistic EoS to address such phase transition. Both ms and n constrain the EoS, making it softer as ms increases. Solutions to the TOV equations reveal that for massless strange quarks, maximum mass is 2.01 M and corresponding radius is 10.96 Km when n=0.66~fm-3. These values decrease to 1.99 M and 1.96 M, with corresponding radii of 10.88 Km and 10.69 Km for ms=50 and 100~MeV respectively having same n value. It is interesting to note that a corelation exists between n and ms. The hadronic to quark matter transition occurs at higher values of n, when ms increases such as n≥0.484,~0.489 and 0.51~fm-3 for ms=50 and 100~MeV respectively. Beyond these values, the energy per baryon (EB) drops below 930.4~MeV, indicating a complete transition to quark matter. For physical analysis, we have considered n~(=0.578~fm-3) which lies in the stable region with B(n)=70~MeV/fm3. The model provides a viable description of strange stars, satisfying all necessary physical requirements.
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