Abstract
Assuming that the order parameter corresponds to an equal spin triplet pairing symmetry state, we calculate the effect of phase fluctuations in quasi-one-dimensional superconductors at high magnetic fields applied along the y ${(b}^{\ensuremath{'}})$ axis. We show that phase fluctuations can destroy the theoretically predicted triplet reentrant superconducting state, and that they are responsible for melting the magnetic-field induced Josephson vortex lattice, above a magnetic-field dependent melting temperature ${T}_{m}.$
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