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Mass-Induced Crystalline Color Superconductivity

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arxiv hep-ph/0112206 v2 pith:ZNQ3JMTK submitted 2001-12-14 hep-ph nucl-th

classification hep-phnucl-th
keywords deltacolorcrystallinesuperconductivityeffectpairingphasequarks
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We demonstrate that crystalline color superconductivity may arise as a result of pairing between massless quarks and quarks with nonzero mass m_s. Previous analyses of this phase of cold dense quark matter have all utilized a chemical potential difference \delta\mu to favor crystalline color superconductivity over ordinary BCS pairing. In any context in which crystalline color superconductivity occurs in nature, however, it will be m_s-induced. The effect of m_s is qualitatively different from that of \delta\mu in one crucial respect: m_s depresses the value of the BCS gap \Delta_0 whereas \delta\mu leaves \Delta_0 unchanged. This effect in the BCS phase must be taken into account before m_s-induced and \delta\mu-induced crystalline color superconductivity can sensibly be compared.

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  1. Berry Curvature and Spin-One Color Superconductivity

    nucl-th 2024-11 conditional novelty 7.0 of 10

    In spin-one color superconductors, the topological node count is set by a generalized pairing monopole charge that includes color Berry flux, which cancels in the color-spin-locking phase and produces gapless quasipar...

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