Table 1 Relevant parameters for all the measured devices before and after the thermal cycle
From: Induced unconventional superconductivity on the surface states of Bi2Te3 topological insulator
\({\boldsymbol{I}}_{\bf{C}}^{{\bf{before}}}\) | \({\boldsymbol{I}}_{\bf {C}}^{{{\bf after}}}\) | \({\boldsymbol{R}}_{{\bf N}}^{{{\bf before}}}\) | \({\boldsymbol{R}}_{{\bf N}}^{{{\bf after}}}\) | \({\boldsymbol{I}}_{{\bf C}}{\boldsymbol{R}}_{{\bf N}}^{{{\bf before}}}\) | \({\boldsymbol{I}}_{{\bf C}}{\boldsymbol{R}}_{{\bf N}}^{{{\bf after}}}\) | w | L | \(\frac{{{\boldsymbol{I}}_{{\bf C}}^{{{\bf after}}}}}{{{\boldsymbol{I}}_{{\bf C}}^{{{\bf before}}}}}\) | \(\frac{{{\boldsymbol{R}}_{{\bf N}}^{{{\bf after}}}}}{{{\boldsymbol{R}}_{{\bf N}}^{{{\bf before}}}}}\) | |
---|---|---|---|---|---|---|---|---|---|---|
Device | (μA) | (μA) | (Ω) | (Ω) | (μeV) | (μeV) | (μm) | (nm) | ||
JM10 | 2.6 | 0.002 | 36 | 215 | 89 | 0.4 | 1 | 200 | 0.07% | 6.0 |
JM5 | — | 0.017 | — | 216 | — | 3.6 | 0.5 | 100 | — | — |
JM11 | 1.8 | 0.085 | 41 | 62 | 47 | 5 | 1 | 300 | 4% | 1.5 |
SF2 | 0.58 | 0 | 15 | 20 | 9 | 0 | 2 | 100 | 0% | 1.3 |
JM1 | 0.6 | — | 86 | — | 54 | — | 0.5 | 200 | — | — |
SM4 | 9.3 | 0.060 | 17 | 61 | 144 | 8.6 | 1.5 | 100 | 0.6% | 3.6 |
SD3 | 0.36 | 0.040 | 18 | 53 | 6 | 2 | 2 | 250 | 11% | 2.9 |
SF3 | 2.2 | 0.030 | 10 | 25 | 22 | 0.7 | 2 | 100 | 1.4% | 2.5 |
SF8 | 3.2 | 0.180 | 11 | 25 | 35 | 4.5 | 2 | 100 | 5.6% | 2.3 |
SD4 | 0.6 | 0.02 | 32 | 52 (59) | 2 | 1 | 2 | 250 | 3% | 1.6 |
SF4 | 19.8 | 6.600 | 3.6 | 5.6 | — | — | 6 | 100 | 33% | 1.5 |
SD2 | 0.52 | 0.012 | 17 | 20 (73) | 9 | 0.2 | 4 | 250 | 2.3% | 1.2 |
SD1 | 1.2 | 0.086 | 27 | 30 | 32 | 2.5 | 2 | 250 | 7.1% | 1.1 |
SM1 | 11.0 | — | 15 | — | 151 | — | 1.5 | 100 | — | — |