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When the vortex lattice with a modulation induced by the paramagnetic depairing has, in contrast to the case of CeCo In5, nodal planes parallel to H, the structural transitions between Josephson vortex lattices play important roles even if this inequality 9 is satisfied. This case is relevant to the corresponding issue in λ- (BET)2 Fe Cl4 [PRLTAO 0031-9007 10.1103/PhysRevLett.97.157001
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When the vortex lattice with a modulation induced by the paramagnetic depairing has, in contrast to the case of CeCo In5, nodal planes parallel to H, the structural transitions between Josephson vortex lattices play important roles even if this inequality 9 is satisfied. This case is relevant to the corresponding issue in λ- (BET)2 Fe Cl4 [S. Uji, T. Terashima, M. Nishimura, Y. Takahide, T. Konoike, K. Enomoto, H. Cui, H. Kobayashi, A. Kobayashi, H. Tanaka, M. Tokumoto, E. S. Choi, T. Tokumoto, D. Graf, and J. S. Brooks, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.97.157001 97, 157001 (2006)] and will be discussed elsewhere [arXiv:cond-mat/0708.2137].
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We stress that a kink anomaly (Ref.) at HFFLO in the thermal conductivity for a heat current-H should appear even when the nodal planes are perpendicular to the vortex lines because, in GL region, the thermal conductivity usually increases as, just like in entering the FFLO state by increasing the field (Ref.), the gap amplitude is reduced. See, for instance, the work by PKOMA3 0031-9236 10.1007/BF02422842
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