Altermagnetic spin splitting selects direction-selective triplet pairing in 2D d-wave metals and generates spin-locked Majorana edge states in both spin-conserving and Rashba-mixed regimes.
Title resolution pending
3 Pith papers cite this work. Polarity classification is still indexing.
3
Pith papers citing it
verdicts
UNVERDICTED 3representative citing papers
Fe-based superconductors with coplanar magnetic order realize an odd-parity magnetic state featuring k_z-polarized spins with h-wave splitting and finite Berry curvature but vanishing Edelstein effect in the absence of spin-orbit coupling.
Zeeman field controls competition between superconductivity and disorder in helical edges, with disorder causing logarithmic suppression of density-wave correlations and positive corrections that stabilize superconducting pairs, altering spin conductance scaling.
citing papers explorer
-
Direction-selective triplet pairing and spin-edge locking in altermagnetic metals
Altermagnetic spin splitting selects direction-selective triplet pairing in 2D d-wave metals and generates spin-locked Majorana edge states in both spin-conserving and Rashba-mixed regimes.
-
Odd-Parity Magnetism in Fe-Based Superconductors
Fe-based superconductors with coplanar magnetic order realize an odd-parity magnetic state featuring k_z-polarized spins with h-wave splitting and finite Berry curvature but vanishing Edelstein effect in the absence of spin-orbit coupling.
-
Spin responses of a disordered helical superconducting edge under Zeeman field
Zeeman field controls competition between superconductivity and disorder in helical edges, with disorder causing logarithmic suppression of density-wave correlations and positive corrections that stabilize superconducting pairs, altering spin conductance scaling.