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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In anisotropic disordered 2D metals, altermagnetism emerges at zero temperature for larger anisotropy and coupling strengths, competing with ferromagnetism at zero spin-orbit coupling and with a paramagnetic phase at finite spin-orbit coupling via a quantum critical point.
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.
Strong correlations in a Josephson junction with odd electrons spontaneously break symmetries to enable zero-field Josephson diode effect without magnetic order.
citing papers explorer
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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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Quantum Altermagnetic Instability in Disordered Metals
In anisotropic disordered 2D metals, altermagnetism emerges at zero temperature for larger anisotropy and coupling strengths, competing with ferromagnetism at zero spin-orbit coupling and with a paramagnetic phase at finite spin-orbit coupling via a quantum critical point.
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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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Strong Correlation Drives Zero-Field Josephson Diode Effect
Strong correlations in a Josephson junction with odd electrons spontaneously break symmetries to enable zero-field Josephson diode effect without magnetic order.