Complete zero-energy flat bands of surface states in fully gapped chiral noncentrosymmetric superconductors
Source abstract
Abstract
Flat bands of surface states in noncentrosymmetric superconductors accompanied by a full gap in the bulk would be an alternative route to a strongly interacting two-dimensional Fermi system. They could provide a robust platform for quantum computation. Here, the authors explore a way to stabilize such bands in the entire surface Brillouin zone by introducing an additional spin-rotation symmetry that forces the direction of the spin-orbit-coupling vector not to depend on the momentum component, normal to the surface.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Topological Materials and Phenomena · Advanced Condensed Matter Physics · Rare-earth and actinide compounds
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Institute of Theoretical Physics, Technische Universität Dresden, 01069 Dresden, Germany and Würzburg–Dresden Cluster of Excellence ct.qmat, Technische Universität Dresden, 01062 Dresden, Germany
Funding
Deutsche Forschungsgemeinschaft
References (44)
Show source-provided references
1. 10.1103/PhysRevB.84.06050410.1103/PhysRevB.84.060504 ↗
2. 10.1103/PhysRevB.84.02050110.1103/PhysRevB.84.020501 ↗
3. 10.1103/PhysRevB.83.22451110.1103/PhysRevB.83.224511 ↗
4. 10.1103/PhysRevB.85.02452210.1103/PhysRevB.85.024522 ↗
5. 10.1103/PhysRevB.88.13450510.1103/PhysRevB.88.134505 ↗
6. 10.1088/0953-8984/27/24/24320110.1088/0953-8984/27/24/243201 ↗
7. 10.1016/S0003-4916(02)00018-010.1016/S0003-4916(02)00018-0 ↗
8. 10.1103/RevModPhys.80.108310.1103/RevModPhys.80.1083 ↗
9. 10.1103/PhysRevLett.104.04050210.1103/PhysRevLett.104.040502 ↗
10. 10.1103/PhysRevLett.105.07700110.1103/PhysRevLett.105.077001 ↗
11. 10.1103/PhysRevLett.105.17700210.1103/PhysRevLett.105.177002 ↗
12. 10.1088/1367-2630/15/4/04501910.1088/1367-2630/15/4/045019 ↗
13. 10.1103/RevModPhys.87.13710.1103/RevModPhys.87.137 ↗
14. 10.1038/npjqi.2015.110.1038/npjqi.2015.1 ↗
15. 10.1146/annurev-conmatphys-031218-01361810.1146/annurev-conmatphys-031218-013618 ↗
16. 10.1103/PhysRevB.101.02451910.1103/PhysRevB.101.024519 ↗
17. 10.1103/PhysRevB.105.18450110.1103/PhysRevB.105.184501 ↗
18. 10.1103/PhysRevLett.112.11700210.1103/PhysRevLett.112.117002 ↗
19. 10.1103/PhysRevB.91.16540210.1103/PhysRevB.91.165402 ↗
20. 10.1103/PhysRevB.108.22450310.1103/PhysRevB.108.224503 ↗
21. 10.1103/PhysRevB.103.24511510.1103/PhysRevB.103.245115 ↗
22. 10.1103/PhysRevB.78.19512510.1103/PhysRevB.78.195125 ↗
23. 10.1103/PhysRevB.55.114210.1103/PhysRevB.55.1142 ↗
24. 10.1063/1.53167510.1063/1.531675 ↗
25. 10.1103/PhysRevLett.92.09700110.1103/PhysRevLett.92.097001 ↗
26. 10.1016/j.aop.2009.08.00810.1016/j.aop.2009.08.008 ↗
27. 10.1088/1361-6633/80/3/03650110.1088/1361-6633/80/3/036501 ↗
28. 10.1143/JPSJ.78.03471010.1143/JPSJ.78.034710 ↗
29. 10.1103/PhysRevB.87.22450210.1103/PhysRevB.87.224502 ↗
30. 10.1103/PhysRevB.84.06451810.1103/PhysRevB.84.064518 ↗
31. 10.1103/PhysRevB.86.09452010.1103/PhysRevB.86.094520 ↗
32. 10.7566/JPSJ.82.08471110.7566/JPSJ.82.084711 ↗
33. 10.1088/0953-8984/16/4/L0210.1088/0953-8984/16/4/L02 ↗
34. 10.1143/JPSJ.73.312910.1143/JPSJ.73.3129 ↗
35. 10.1016/j.physb.2006.01.12610.1016/j.physb.2006.01.126 ↗
36. 10.1143/JPSJ.78.08472410.1143/JPSJ.78.084724 ↗
37. 10.1088/1367-2630/15/5/05300510.1088/1367-2630/15/5/053005 ↗
38. 10.1088/0953-2048/27/3/03500410.1088/0953-2048/27/3/035004 ↗
39. 10.1126/sciadv.aar796910.1126/sciadv.aar7969 ↗
40. 10.1103/PhysRevB.104.22450810.1103/PhysRevB.104.224508 ↗
41. 10.1103/PhysRevLett.111.07700110.1103/PhysRevLett.111.077001 ↗
42. 10.1088/1367-2630/17/1/01301610.1088/1367-2630/17/1/013016 ↗
43. 10.1103/PhysRevLett.105.09700210.1103/PhysRevLett.105.097002 ↗
44. 10.1103/PhysRevB.91.18050310.1103/PhysRevB.91.180503 ↗