Table 1 Irreducible representations (ireps) of point group D6 (θ ≠ 30) and D6d (θ = 30).

From: Non-Abelian topological superconductivity in maximally twisted double-layer spin-triplet valley-singlet superconductors

Group

IR

cubic functions

SC order parameters

D6

A1

\({\psi }_{1}{\psi }_{2}^{* }+{\psi }_{1}^{* }{\psi }_{2}\), \({\psi }_{1}^{2}{\psi }_{2}^{* 2}+{\psi }_{1}^{* 2}{\psi }_{2}^{2}\)

 

B1

x3 − 3xy2

ψ1 + ψ2

 

B2

3x2y − y3

ψ1 − ψ2

D6d

A1

\({\psi }_{1}^{2}{\psi }_{2}^{* 2}+{\psi }_{1}^{* 2}{\psi }_{2}^{2}\)

 

E3

{x3 − 3xy2, 3x2y − y3}

{ψ1 + ψ2, ψ1 − ψ2}

  1. Basis functions include cubic functions and reconstructed f-wave superconducting (SC) order parameters ψ1, ψ2 in the moiré bands in twisted double-layer. Symmetry properties of ψ1, ψ2 are derived from Eq. (16). A1 is the trivial irep in both cases.