Phase fluctuations of s-wave superconductors on a lattice
arXiv:cond-mat/0309261 · doi:10.1023/B:JOLT.0000024550.59637.c2
Abstract
Based on an attractive Hubbard model on a lattice with up to second neighbor hopping we derive an effective Hamiltonian for phase fluctuations. The superconducting gap is assumed to have s-wave symmetry. The effective Hamiltonian we finally arrive at is of the extended XY type. While it correctly reduces to a simple XY in the continuum limit, in the general case, it contains higher neighbor interaction in spin space. An important feature of our Hamiltonian is that it gives a much larger fluctuation region between the Berezinskii-Kosterlitz-Thouless transition temperature identified with for superconducting and the mean field transition temperature identified with the pseudogap temperature.
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References in corpus (7)
- Phase Fluctuations and Pseudogap Phenomena
- QED3 theory of pairing pseudogap in cuprates: From d-wave superconductor to antiferromagnet via "algebraic" Fermi liquid
- Finite Temperature Time-Dependent Effective Theory for the Phase Field in two-dimensional d-wave Neutral Superconductor
- Transport properties in the d-density wave state: Wiedemann-Franz law
- Phase fluctuations in superconductors: from Galilean invariant to quantum XY models
- An effective Hamiltonian for phase fluctuations on a lattice: an extended XY model
- Nodal quasiparticles and classical phase fluctuations in d-wave superconductors