Abstract

We compute free energy of quark matter at asymptotically high baryon number density in the presence of nonzero strange quark mass including dynamics of pseudo Nambu-Goldstone bosons due to chiral symmetry breaking, extending previously existing analysis based on perturbative expansion in ${m}_{s}^{2}/4\ensuremath{\mu}\ensuremath{\Delta}.$ We demonstrate that the $\mathrm{C}\mathrm{F}\mathrm{L}{K}^{0}$ state has lower free energy than the symmetric CFL state for $0<{m}_{s}^{2}/4\ensuremath{\mu}\ensuremath{\Delta}<2/3$. We also calculate the spectrum of the fermionic quasiparticle excitations about the kaon condensed ground state in the regime ${m}_{s}^{2}/4\ensuremath{\mu}\ensuremath{\Delta}\ensuremath{\sim}1$ and find that $({m}_{s}^{2}/4\ensuremath{\mu}\ensuremath{\Delta}{)}_{\mathrm{c}\mathrm{r}\mathrm{i}\mathrm{t}}=2/3$ for the CFL-gCFL phase transition, the leading order result reported in [20], is not modified.

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