Soft loop-current fluctuations involving vanadium and antimony orbitals in kagome metals mediate chiral d+id and disorder-robust s± pairing channels, with a pressure-driven Lifshitz transition selecting between them.
Title resolution pending
3 Pith papers cite this work. Polarity classification is still indexing.
3
Pith papers citing it
verdicts
UNVERDICTED 3representative citing papers
A Ginzburg-Landau stacking analysis of the 2x2x4 CDW in CsV3Sb5 identifies chiral inversion-breaking phases when layer rigidity is relaxed, yet these phases remain rare in the phase diagram.
Ti hole-doping suppresses competing 2x2x2 and 2x2x4 charge density wave supercells in the first superconducting dome of CsV3-xTixSb5 while eliminating detectable charge correlations in the second dome, leaving superconductivity conventional and distinct from Sb-site Sn doping.
citing papers explorer
-
Superconductivity in kagome metals due to soft loop-current fluctuations
Soft loop-current fluctuations involving vanadium and antimony orbitals in kagome metals mediate chiral d+id and disorder-robust s± pairing channels, with a pressure-driven Lifshitz transition selecting between them.
-
Four-layer charge density waves and chirality in CsV$_3$Sb$_5$
A Ginzburg-Landau stacking analysis of the 2x2x4 CDW in CsV3Sb5 identifies chiral inversion-breaking phases when layer rigidity is relaxed, yet these phases remain rare in the phase diagram.
-
Evolution of charge correlations in the hole-doped kagome superconductor CsV$_{3-x}$Ti$_x$Sb$_5$
Ti hole-doping suppresses competing 2x2x2 and 2x2x4 charge density wave supercells in the first superconducting dome of CsV3-xTixSb5 while eliminating detectable charge correlations in the second dome, leaving superconductivity conventional and distinct from Sb-site Sn doping.