Floating Majorana edge bands in d-wave proximitized quantum anomalous Hall insulators produce quantized thermal conductance that remains stable under disorder and finite temperature.
Title resolution pending
5 Pith papers cite this work. Polarity classification is still indexing.
citation-role summary
citation-polarity summary
roles
background 1polarities
background 1representative citing papers
Odd-parity altermagnetism reconstructs local topology in the Chern-insulating phase of the Haldane-Hubbard model without changing the total Chern number.
Treating orbital degrees of freedom as dynamical variables in altermagnets generates emergent electric fields tunable by lattice anisotropy, driving orbital and magnetic multipole currents even in simplified textures with dynamic lattice distortion.
Floquet engineering with periodic light fields induces odd-parity magnetism and tunable spin splitting in 2D collinear antiferromagnets.
citing papers explorer
-
Robust quantized thermal conductance of Majorana floating edge bands in d-wave superconductors
Floating Majorana edge bands in d-wave proximitized quantum anomalous Hall insulators produce quantized thermal conductance that remains stable under disorder and finite temperature.
-
The odd-parity altermagnetism induced reconstruction of the Chern-insulating phase in Haldane-Hubbard model
Odd-parity altermagnetism reconstructs local topology in the Chern-insulating phase of the Haldane-Hubbard model without changing the total Chern number.
-
Orbital-driven emergent transport in altermagnets
Treating orbital degrees of freedom as dynamical variables in altermagnets generates emergent electric fields tunable by lattice anisotropy, driving orbital and magnetic multipole currents even in simplified textures with dynamic lattice distortion.
-
Light-induced Odd-parity Magnetism in Conventional Collinear Antiferromagnets
Floquet engineering with periodic light fields induces odd-parity magnetism and tunable spin splitting in 2D collinear antiferromagnets.
- Nonmagnetic-magnetic Transitions in Rutile RuO2