The zero-temperature Knight shift of a strongly spin-orbit-locked superconductor equals chi_N times (identity minus the Fermi-surface average of the spin-locking projector), independently of pairing symmetry and gap size.
Title resolution pending
4 Pith papers cite this work. Polarity classification is still indexing.
4
Pith papers citing it
representative citing papers
Strong local pairing on the links of a square lattice can trap Cooper pairs in a flat band, giving zero pair kinetic energy and zero superfluid stiffness in the strong-coupling limit.
Weak easy-plane anisotropy generates attractive equal-spin p-wave pairing via two-magnon exchange in a 2D half-metal, with λp enhanced to O(1) near the ferromagnetic onset.
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
-
Bogoliubov sum rule and the Knight-shift ellipsoid in spin-locked superconductors
The zero-temperature Knight shift of a strongly spin-orbit-locked superconductor equals chi_N times (identity minus the Fermi-surface average of the spin-locking projector), independently of pairing symmetry and gap size.
-
Obstructed Cooper pairs in flat band systems -- weakly-coherent superfluids and exact spin liquids
Strong local pairing on the links of a square lattice can trap Cooper pairs in a flat band, giving zero pair kinetic energy and zero superfluid stiffness in the strong-coupling limit.
-
Magnon-Mediated Superconductivity in a 2D Itinerant Ferromagnet with Weak Easy-plane Magnetic Anisotropy
Weak easy-plane anisotropy generates attractive equal-spin p-wave pairing via two-magnon exchange in a 2D half-metal, with λp enhanced to O(1) near the ferromagnetic onset.
-
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.