Single Spin Superconductivity: Formulation and Ginzburg-Landau Theory
Robert E. Rudd, Warren E. Pickett

TL;DR
This paper introduces a new type of superconductivity arising from a pairing instability in half-metallic antiferromagnetic states, with a detailed symmetry-based Ginzburg-Landau theory and phase diagram analysis.
Contribution
It formulates the Ginzburg-Landau theory for single spin superconductivity and classifies possible phases based on symmetry considerations.
Findings
Identifies the least symmetric normal phase allowing zero momentum pairing.
Constructs a symmetry-consistent Ginzburg-Landau free energy for various crystal point groups.
Predicts gap nodes leading to power-law thermodynamic behavior at low temperatures.
Abstract
We describe a novel superconducting phase that arises due to a pairing instability of the half-metallic antiferromagnetic (HM AFM) normal state. This single spin superconducting (SSS) phase contains broken time reversal symmetry in addition to broken gauge symmetry, the former due to the underlying magnetic order in the normal state. A classification of normal state symmetries leads to the conclusion that the HM AFM normal phase whose point group contains the inversion operator contains the least symmetry possible which still allows for a zero momentum pairing instability. The Ginzburg-Landau free energy for the superconducting order parameter is constructed consistent with the symmetry of the normal phase, electromagnetic gauge invariance and the crystallographic point group symmetry including inversion. For cubic, hexagonal and tetragonal point groups, the possible symmetries of the…
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