Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
Title resolution pending
4 Pith papers cite this work. Polarity classification is still indexing.
4
Pith papers citing it
citation-role summary
background 1
citation-polarity summary
years
2026 4verdicts
UNVERDICTED 4roles
background 1polarities
background 1representative citing papers
Altermagnets host a purely intrinsic orbital-splitter current that is strongly anisotropic, exceeds the spin-splitter current by up to a factor of four in some directions, and generates damping-like torque to speed up magnetization switching.
Altermagnets host a giant nonperturbative magnetic orbital Hall effect that generates collinear orbital currents capable of switching perpendicular magnetization without external fields.
A weak crystal potential in d-wave altermagnets induces real-space spin quadrupolar order without unit cell enlargement.
citing papers explorer
-
Nodal Topological Superconductivity Driven by Crystalline Antiunitary Symmetry in Altermagnets
Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
-
Orbital-Splitter Current in Altermagnets
Altermagnets host a purely intrinsic orbital-splitter current that is strongly anisotropic, exceeds the spin-splitter current by up to a factor of four in some directions, and generates damping-like torque to speed up magnetization switching.
-
Nonperturbative Magnetic Orbital Hall Effect in Altermagnets
Altermagnets host a giant nonperturbative magnetic orbital Hall effect that generates collinear orbital currents capable of switching perpendicular magnetization without external fields.
-
Spin Quadrupolar orders in $d$-wave Unconventional Magnetism
A weak crystal potential in d-wave altermagnets induces real-space spin quadrupolar order without unit cell enlargement.