[1810.12308] Rotation Symmetry-Protected Topological Phases of Fermions
[1810.12314] Knotted Non-Hermitian Metals
[1810.12317] Intrinsically interacting topological crystalline insulators and superconductors
[1810.12332] Three dimensional collective charge excitations in electron-doped cuprate superconductors
[1810.12524] The Many Faces of Far-from-equilibrium Thermodynamics: Deterministic Chaos, Randomness or Emergent Order?
[1810.12601] Topological classification under nonmagnetic and magnetic point group symmetry: application of Atiyah-Hirzebruch spectral sequence to higer-order topology
[1810.12700] Machine learning density functional theory for the Hubbard model
[1810.12899] Anomalous symmetry protected topological states in interacting fermion systems
[1810.12550] The Connection of Topology between Systems with Different Dimensions: 1D Zak Phases to 2D Chern Number, Weyl Point as the Jumping Channel for One Singularity and Nodal Line to Merge All Singularities
[1810.12314] Knotted Non-Hermitian Metals
[1810.12317] Intrinsically interacting topological crystalline insulators and superconductors
[1810.12332] Three dimensional collective charge excitations in electron-doped cuprate superconductors
[1810.12524] The Many Faces of Far-from-equilibrium Thermodynamics: Deterministic Chaos, Randomness or Emergent Order?
[1810.12601] Topological classification under nonmagnetic and magnetic point group symmetry: application of Atiyah-Hirzebruch spectral sequence to higer-order topology
[1810.12700] Machine learning density functional theory for the Hubbard model
[1810.12899] Anomalous symmetry protected topological states in interacting fermion systems
[1810.12550] The Connection of Topology between Systems with Different Dimensions: 1D Zak Phases to 2D Chern Number, Weyl Point as the Jumping Channel for One Singularity and Nodal Line to Merge All Singularities