Table 2 Leading superconducting states in the flat-band limit, following from Eq. (7), for pairing mediated by fluctuations of the indicated orders, defined by using λj in Eq. (4)

From: Nodal band-off-diagonal superconductivity in twisted graphene superlattices

Fluctuating order

Leading superconductor

type

λj

\({\bar{\lambda }}^{j}\)

\({{{\Delta }}}_{{{{{{{{\boldsymbol{k}}}}}}}},\eta }^{}\)

IR

T-IVC

σ0ηx,y

ρxηx,y

σyδk

A2

K-IVC

σyηx,y

ρyηx,y

σ0ηδk

B1

SLP + 

σyηz

ρzη0

σyδk, σ0ηδk

A2, B1

SLP − 

σyη0

ρzηz

σxηδk, σzηδk

B2, B1

  1. Here, δk > 0 and states separated by commas are degenerate. The couplings in the microscopic basis, used in Fig. 4 for the respective orders, are listed under \({\bar{\lambda }}^{j}\). Except for SLP−, the leading superconducting states for λj and \({\bar{\lambda }}^{j}\) are the same (cf. Fig. 4 and Supplementary Appendix D1).
Back to article page