journal article·2020-07-30

Nodeless superconducting gap in the topological superconductor candidate 2M–WS2

L. S. Wang, Y. Q. Fang, Y. Y. Huang, E. J. Cheng, J. M. Ni, B. L. Pan, Y. Xu, F. Q. Huang, S. Y. Li

Physical Review B· Volume 102· Issue 2
Publisher page

Abstract

Recently, a new transition-metal dichalcogenide (TMD) material $2M$-phase ${\mathrm{WS}}2$ was synthesized. The material $2M\text{\ensuremath{-}}{\mathrm{WS}}2$ not only exhibits superconductivity, with the highest ${T}_{\text{c}}$ being 8.8 K at ambient pressure among TMDs, but also hosts a topological surface state. Here we report the low-temperature thermal conductivity measurements on $2M\text{\ensuremath{-}}{\mathrm{WS}}2$ single crystals to investigate its superconducting gap structure. A negligible residual linear term ${\ensuremath{\kappa}}0/T$ in zero field shows that $2M\text{\ensuremath{-}}{\mathrm{WS}}2$ has a fully superconducting gap with all electrons paired. The field dependence of ${\ensuremath{\kappa}}0/T$ suggests an anisotropic superconducting gap or multiple nodeless superconducting gaps in $2M\text{\ensuremath{-}}{\mathrm{WS}}2$. Such a fully gapped superconducting state is compatible with $2M\text{\ensuremath{-}}{\mathrm{WS}}2$ being a topological superconductor candidate.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: 2D Materials and Applications · Topological Materials and Phenomena · Graphene research and applications

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (43)

Show source-provided references
1. 10.1103/RevModPhys.83.105710.1103/RevModPhys.83.1057 ↗
2. 10.1103/RevModPhys.80.108310.1103/RevModPhys.80.1083 ↗
3. 10.1088/1361-6633/aa6ac710.1088/1361-6633/aa6ac7 ↗
4. 10.1088/0034-4885/75/4/04250110.1088/0034-4885/75/4/042501 ↗
5. 10.1088/0034-4885/79/5/05450210.1088/0034-4885/79/5/054502 ↗
6. 10.1038/s41586-019-1596-210.1038/s41586-019-1596-2 ↗
7. 10.1103/PhysRevLett.100.09640710.1103/PhysRevLett.100.096407 ↗
8. 10.1126/science.121646610.1126/science.1216466 ↗
9. 10.1038/nphys313910.1038/nphys3139 ↗
10. 10.1103/PhysRevLett.114.01700110.1103/PhysRevLett.114.017001 ↗
11. 10.1103/PhysRevLett.112.21700110.1103/PhysRevLett.112.217001 ↗
12. 10.1093/nsr/nwy14210.1093/nsr/nwy142 ↗
13. 10.1103/PhysRevLett.117.04700110.1103/PhysRevLett.117.047001 ↗
14. 10.1103/PhysRevB.92.11511910.1103/PhysRevB.92.115119 ↗
15. 10.1038/s41567-018-0280-z10.1038/s41567-018-0280-z ↗
16. 10.1126/science.aao179710.1126/science.aao1797 ↗
17. 10.1126/science.aan459610.1126/science.aan4596 ↗
18. 10.1103/PhysRevX.8.04105610.1103/PhysRevX.8.041056 ↗
19. 10.1038/nphys337110.1038/nphys3371 ↗
20. 10.1038/ncomms1397310.1038/ncomms13973 ↗
21. 10.1038/nphys387110.1038/nphys3871 ↗
22. 10.1038/nphys417410.1038/nphys4174 ↗
23. 10.1002/adma.20190194210.1002/adma.201901942 ↗
24. 10.1038/s41567-019-0576-710.1038/s41567-019-0576-7 ↗
25. 10.1038/s41535-019-0189-510.1038/s41535-019-0189-5 ↗
26. 10.1088/1367-2630/11/5/05506510.1088/1367-2630/11/5/055065 ↗
27. 10.1103/PhysRev.136.A16610.1103/PhysRev.136.A166 ↗
28. 10.1103/PhysRevLett.103.23640110.1103/PhysRevLett.103.236401 ↗
29. 10.1103/PhysRevB.92.18050510.1103/PhysRevB.92.180505 ↗
30. 10.1038/nmat437410.1038/nmat4374 ↗
31. 10.1038/nphys353810.1038/nphys3538 ↗
32. M. Tinkham · 1996
33. 10.1038/s41467-017-00427-510.1038/s41467-017-00427-5 ↗
34. 10.1103/PhysRevB.82.01451810.1103/PhysRevB.82.014518 ↗
35. 10.1103/PhysRevB.77.13450110.1103/PhysRevB.77.134501 ↗
36. 10.1103/PhysRevB.67.17452010.1103/PhysRevB.67.174520 ↗
37. 10.1103/PhysRevB.14.191610.1103/PhysRevB.14.1916 ↗
38. 10.1103/PhysRevLett.90.11700310.1103/PhysRevLett.90.117003 ↗
39. 10.1103/PhysRevLett.89.14700310.1103/PhysRevLett.89.147003 ↗
40. 10.1103/PhysRevB.98.10450610.1103/PhysRevB.98.104506 ↗
41. 10.1103/PhysRevLett.110.11700110.1103/PhysRevLett.110.117001 ↗
42. 10.1103/PhysRevLett.107.21700110.1103/PhysRevLett.107.217001 ↗
43. 10.1103/PhysRevLett.106.12700410.1103/PhysRevLett.106.127004 ↗