Table 1 Deduced parameters for single-band models applied to MATBG sample M27 doped at nn = −1.44 1012 cm−2 where an effective mass of charge carriers m*/me = 0.1637 ± 0.0154 was used, which was obtained from the analysis presented in Fig. 5.

From: Classifying superconductivity in Moiré graphene superlattices

Model

Tc (K)

Δ(0) (μeV)

2Δ(0)/kBTc

ΔC/C

vF (104 m/s)

TF (K)

Tc/TF

λ(0) (nm)

s-wave

1.28 ± 0.05

245 ± 9

4.4 ± 0.2

2.7 ±0.9

7.3 ± 0.3

28.6 ± 2.0

0.045 ± 0.002

2,182 ± 3

d-wave (low-T asymptote)

 

2,300 ± 500

>40

    

2,166 ± 5

p-wave polar Al

1.24 ± 0.06

>106

>104

>7

   

2,142 ± 25

p-wave polar A||l

1.34 ± 0.05

430 ± 32

7.4 ± 0.6

1.0 ± 0.3

13 ± 1

86 ± 15

0.015 ± 0.003

2,180 ± 3

p-wave axial Al

1.31 ± 0.05

301 ± 13

5.4 ± 0.2

1.9 ± 0.6

8.8 ± 0.3

42 ± 3

0.031 ± 0.002

2,183 ± 3

p-wave axial A||l

1.37 ± 0.05

1,500 ± 1,200

27 ± 22

2.3 ± 0.5

46

1,100

>0.001

2,178 ± 3

d + id-wave

1.27 ± 0.05

Gap 1

322 ± 38

5.92 ± 0.70

0.959 (fixed)

9.5 ± 1.0

49 ± 10

0.026 ± 0.003

2,180 ± 3

Gap 2

187 ± 24

3.44 ± 0.30

0.959 (fixed)

5.5 ± 0.5

16 ± 3

0.078 ± 0.016

  1. For the case of d + id we fixed the ratio of ΔC/C = 0.995 for both gaps. The ground-state coherence length was assumed to be ξ(0) = 61.4 ± 1.7 nm.