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Phys. Rev. Lett. 96, 012305 (2006) [4 pages]

Meson Supercurrent State in High-Density QCD

T. Schäfer
Department of Physics, North Carolina State University, Raleigh, North Carolina 27695, USA
Received 31 August 2005; published 12 January 2006

The ground state of three flavor quark matter at asymptotically large density is believed to be the color-flavor-locked (CFL) phase. At nonasymptotic density the effect of the nonzero strange quark mass cannot be neglected. If the strange quark mass exceeds ms~m<sub>u</sub><sup>1/3</sup>Delta2/3, the CFL state becomes unstable toward the formation of a neutral kaon condensate. Recently, several authors discovered that for ms~(2DeltapF)1/2 the CFL state contains gapless fermions, and that the gapless modes lead to an instability in current-current correlation functions. Using an effective theory of the CFL state, we demonstrate that this instability can be resolved by the formation of a meson supercurrent, analogous to Migdal's p-wave pion condensate. This state has a nonzero meson current that is canceled by a backflow of gapless fermions.

©2006 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevLett.96.012305
DOI: 10.1103/PhysRevLett.96.012305
PACS: 12.38.Mh
  • 12.38.Mh
    Quark–gluon plasma
  • YEAR: 2006
KEYWORDS: quantum chromodynamics, quark mass, strange particles, current algebra, flavour model, quark matter, fermions

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