Symmetry matching between altermagnets and unconventional superconductors generates bulk zero-energy flat bands as Bogoliubov Fermi surfaces and distinct curved or flat surface states detectable by tunneling.
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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.
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Engineering subgap states in superconductors by the symmetry of altermagnetism
Symmetry matching between altermagnets and unconventional superconductors generates bulk zero-energy flat bands as Bogoliubov Fermi surfaces and distinct curved or flat surface states detectable by tunneling.
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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.