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Rev. D 64, 074017 (2001) [arXiv:hep-ph/0105009]. 77. A. Gerhold and A. Rebhan, Phys. Rev. D 68, 011502 (2003) [arXiv:hep-ph/0305108]; A. Kryjevski, Phys. Rev. D 68, 074008 (2003) [arXiv:hep-ph/0305173]; A. Gerhold, Phys. Rev. D 71, 014039 (2005) [arXiv:hep-ph/0411086]; D. D. Dietrich and D. H. Rischke, Prog. Part. Nucl. Phys. 53, 305 (2004) [arXiv:nucl-th/0312044]; 36 Color Superconductivity in Dense Quark Matter 78. R. Casalbuoni, R. Gatto, M. Mannarelli and G. Nardulli, Phys. Rev. D 66, 014006 (2002) [arXiv:hep-ph/0201059].
Nardulli, Phys. Rev. D 66, 094006 (2002) [arXiv:hep-ph/0208121]. 80. A. Sedrakian, arXiv:nucl-th/0312053. 81. D. T. Son and M. A. Stephanov, arXiv:cond-mat/0507586. 82. M. Mannarelli, G. Nardulli and M. Ruggieri, arXiv:cond-mat/0604579. Chapter 2 Larkin-Ovchinnikov-Fulde-Ferrell Phases in QCD Giuseppe Nardulli Department of Physics, University of Bari and INFN-Bari, Via E. it The Larkin-Ovchinnikov-Fulde-Ferrell (LOFF) inhomogeneous color superconducting phase of QCD is reviewed. The case of two flavors is discussed in the hypothesis that the gap is formed by one or more plane waves.
52 The terms that occur in the three-flavor case but not in the two-flavor case, namely ^32 and 7322, describe the interaction between the two condensates and hence depend on the angle