Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
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Altermagnetic sublattice order imposes momentum-dependent nodes in the superconducting gap for local pairing interactions and favors nonunitary equal-spin triplet superconductivity at large spin splitting.
Diode efficiency in Rashba superconductors peaks at the Lifshitz transition to strong helical phases with Bogoliubov Fermi surfaces, while Josephson current anisotropy offers a probe for these surfaces in junctions.
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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.
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Inherent momentum-dependent gap structure of altermagnetic superconductors
Altermagnetic sublattice order imposes momentum-dependent nodes in the superconducting gap for local pairing interactions and favors nonunitary equal-spin triplet superconductivity at large spin splitting.
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Helical phases and Bogoliubov Fermi surfaces probed by superconducting diode effects
Diode efficiency in Rashba superconductors peaks at the Lifshitz transition to strong helical phases with Bogoliubov Fermi surfaces, while Josephson current anisotropy offers a probe for these surfaces in junctions.