Mutual Chern-Simons Theory of Spontaneous Vortex Phase
arXiv:cond-mat/0609525 · doi:10.1103/PhysRevB.76.104502
Abstract
We apply the mutual Chern-Simons effective theory (Phys. Rev. B 71, 235102) of the doped Mott insulator to the study of the so-called spontaneous vortex phase in the low-temperature pseudogap region, which is characterized by strong unconventional superconducting fluctuations. An effective description for the spontaneous vortex phase is derived from the general mutual Chern-Simons Lagrangian, based on which the physical properties including the diamagnetism, spin paramagnetism, magneto-resistance, and the Nernst coefficient, have been quantitatively calculated. The phase boundaries of the spontaneous vortex phase which sits between the onset temperature and the superconducting transition temperature , are also determined within the same framework. The results are consistent with the experimental measurements of the cuprates.
12 pages, 8 figures
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Cited by in corpus (9)
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- Low-Temperature Pseudogap Phenomenon: Precursor of High- Superconductivity
- Superconductivity in Mutual Chern-Simons Gauge Theory
- Crossover from Fermi Arc to Full Fermi Surface
- Thermal Hall Effect and Neutral Spinons in a Doped Mott Insulator
- Mottness, Phase String, and High- Superconductivity
- Electric transport in doped Mott insulators dictated by a non-Ioffe-Larkin composition rule and spinons
- Vortices in a parity-invariant Maxwell-Chern-Simons model
- Self-dual Maxwell-Chern-Simons solitons in a parity-invariant scenario