Obstructed Cooper pairs in the strong-coupling limit on line-graph lattices have identically vanishing leading-order kinetic energy due to frustration, yielding flat bosonic bands, zero superfluid stiffness, and an exact d-wave RVB spin liquid ground state at quarter filling via mapping to the Rokhs
Title resolution pending
3 Pith papers cite this work. Polarity classification is still indexing.
3
Pith papers citing it
verdicts
UNVERDICTED 3representative citing papers
Derives a Bogoliubov sum rule fixing the T=0 Knight shift in noncentrosymmetric superconductors to a Fermi-surface projector of the spin-locking vector, producing a Knight-shift ellipsoid that classifies pairing classes and interprets NMR data.
The work constructs an equivalence class of 3D lattice models realizing single Weyl fermions through symmetry-protected topological states and controlled symmetry breaking, linking them to gapless phases in superconductors and superfluids.
citing papers explorer
-
Obstructed Cooper pairs in flat band systems - weakly-coherent superfluids and exact spin liquids
Obstructed Cooper pairs in the strong-coupling limit on line-graph lattices have identically vanishing leading-order kinetic energy due to frustration, yielding flat bosonic bands, zero superfluid stiffness, and an exact d-wave RVB spin liquid ground state at quarter filling via mapping to the Rokhs
-
Bogoliubov sum rules and the Knight-shift ellipsoid in noncentrosymmetric superconductors
Derives a Bogoliubov sum rule fixing the T=0 Knight shift in noncentrosymmetric superconductors to a Fermi-surface projector of the spin-locking vector, producing a Knight-shift ellipsoid that classifies pairing classes and interprets NMR data.
-
Equivalence class of Emergent Single Weyl fermion lattice models in 3 dimensions: gapless superconductors and superfluids versus chiral fermions
The work constructs an equivalence class of 3D lattice models realizing single Weyl fermions through symmetry-protected topological states and controlled symmetry breaking, linking them to gapless phases in superconductors and superfluids.