Nodeless Versus Nodal Scenarios of Possible Triplet Superconductivity in the Quasi-One-Dimensional Layered Conductor LiMoO
arXiv:1310.0059 · doi:10.1103/PhysRevB.88.094520
Abstract
We consider the problem of the orbital upper critical magnetic field, parallel to the most conducting axis of a quasi-one-dimensional layered superconductor. It is shown that superconductivity can be destroyed through orbital effects at fields much higher than the so-called Clogston-Chandrasekhar paramagnetic limiting field, , provided that superconducting pairing of electrons are of a triplet nature. We demonstrate that the superconducting state of the quasi-one-dimensional layered conductor, , is well described by the suggested theory. To this end, we consider two competing scenarios: 1: a superconducting order parameter without zeros on the Fermi surface, and 2: one with zeros on the Fermi surface - both are shown to lead to destruction of superconductivity at a magnetic field, , five times higher than . With recent experimental measurements on the favoring the nodeless order parameter, we present a strong argument supporting triplet pairing in this compound.
8 pages, 4 figures, 1 table
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- New Luttinger liquid physics from photoemission on LiMoO
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Cited by in corpus (5)
- Spin-triplet superconductivity in a weak-coupling Hubbard model for the quasi-one-dimensional compound LiMoO
- Quantum Limit in a Magnetic Field for Triplet Superconductivity in a Quasi-One-Dimensional Conductor
- Triplet superconductivity in a model of LiMoO
- Possible restoration of superconductivity in the quasi-one-dimensional conductor LiMoO in feasibly high pulsed magnetic fields,
- Wannier-Orbital theory and ARPES for the quasi-1D conductor LiMoO