Edge phase crystals in weak-coupling d-wave superconductors remain the ground state up to roughly half the critical impurity strength, and a uniform edge-current Vorontsov state competes in mesoscopic squares.
Adatom engineering magnetic order in superconductors: Applications to altermagnetic superconductivity
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abstract
We study theoretically how superlattices based on adatoms on surfaces of unconventional superconductors can be used to engineer novel pairing states that break time-reversal symmetry and exhibit non-trivial magnetic point symmetries. We illustrate this using a square-lattice Hubbard model with $d$-wave superconductivity and a subleading $s$-wave state as an example. An adatom superlattice with square-lattice symmetries is shown to stabilize an "orbital-altermagnetic superconductor'', a state that exhibits loop current patterns and associated orbital magnetic moments, which preserve superlattice translations but are odd under four-fold rotations. This state is further characterized by a non-zero Berry curvature quadrupole moment and, upon including spin-orbit coupling, by an altermagnetic spin splitting of the bands and non-trivial spin textures in the superlattice unit cell, with zero net spin moment.
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Impurity strength-temperature phase diagram with phase crystals and competing time-reversal symmetry breaking states in nodal $d$-wave superconductors
Edge phase crystals in weak-coupling d-wave superconductors remain the ground state up to roughly half the critical impurity strength, and a uniform edge-current Vorontsov state competes in mesoscopic squares.