Action of the symmetries on the unit cellR =n1a1 +n2a2↦→n′ 1a1 +n′ 2a2, sublattices (δA, δB)↦→(δ′ A, δ′ B) and spin operators (Sx,S y,S z)≡ (x,y,z )↦→(x′,y′,z′)

( δ′ A, δ′ B) ( x′,y′,z′) E (n1,n 2) ( δA, δB) ( x,y,z ) ˆT (n1,n 2) ( δA, δB) ( −x,−y,−z) C + 3 (−n1−n2,n 1) ( δA− a1, δB− 2a1) ( y,z,x ) C− 3 (n2,−n1−n2) ( δA− a2, δB− 2a2) ( z,x

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it

browse 1 citing papers

representative citing papers

Band representations in Strongly Correlated Settings: The Kitaev Honeycomb Model

cond-mat.str-el · 2025-01-20 · conditional · novelty 6.0

Local spin operators are used as artificial orbitals to construct an effective band structure for the Kitaev spin liquid, and symmetry indicators predict chiral edge modes.

citing papers explorer

Showing 1 of 1 citing paper.

Band representations in Strongly Correlated Settings: The Kitaev Honeycomb Model cond-mat.str-el · 2025-01-20 · conditional · none · ref 2
Local spin operators are used as artificial orbitals to construct an effective band structure for the Kitaev spin liquid, and symmetry indicators predict chiral edge modes.

Action of the symmetries on the unit cellR =n1a1 +n2a2↦→n′ 1a1 +n′ 2a2, sublattices (δA, δB)↦→(δ′ A, δ′ B) and spin operators (Sx,S y,S z)≡ (x,y,z )↦→(x′,y′,z′)

fields

years

verdicts

representative citing papers

citing papers explorer