Pole and zero edge state invariant for one-dimensional non-Hermitian sublattice symmetry
Source abstract
Abstract
There have been several criteria for the existence of topological edge states in 1D non-Hermitian two-band sublattice-symmetric tight-binding Hamiltonians. The generalized Brillouin zone (GBZ) approach uses the integration of the Berry connection over the GBZ contour in the complex wavevector space. An alternate `pole-zero' approach uses algebraic properties of the off-diagonal matrix elements of the sublattice-symmetric Hamiltonian in off-diagonal form. Both correctly predict the presence or absence of edge states, but there has not been an explicit proof of their equivalence. Here we provide such an explicit proof and moreover we extend the pole-zero approach so that it also applies for sublattice-symmetric models when the Hamiltonian is not in off-diagonal form. We give numerical examples for these invariants.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Quantum Mechanics and Non-Hermitian Physics · Topological Materials and Phenomena · Synthesis and Properties of Aromatic Compounds
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Stanford University
Funding
Simons Foundation · U.S. Air Force
References (72)
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1. 10.1103/RevModPhys.82.304510.1103/RevModPhys.82.3045 ↗
2. 10.1103/RevModPhys.88.03500510.1103/RevModPhys.88.035005 ↗
3. 10.1080/00018732.2021.187699110.1080/00018732.2021.1876991 ↗
4. 10.1103/RevModPhys.93.01500510.1103/RevModPhys.93.015005 ↗
5. 10.1038/s42254-022-00516-510.1038/s42254-022-00516-5 ↗
6. 10.1007/s11467-023-1309-z10.1007/s11467-023-1309-z ↗
7. 10.1103/PhysRevLett.121.08680310.1103/PhysRevLett.121.086803 ↗
8. 10.1103/PhysRevLett.123.06640410.1103/PhysRevLett.123.066404 ↗
9. 10.1103/PhysRevB.99.20110310.1103/PhysRevB.99.201103 ↗
10. 10.1103/PhysRevLett.125.22640210.1103/PhysRevLett.125.226402 ↗
11. 10.1038/s42005-024-01519-710.1038/s42005-024-01519-7 ↗
12. 10.22331/q-2021-11-25-59110.22331/q-2021-11-25-591 ↗
13. 10.1103/PhysRevB.107.24540110.1103/PhysRevB.107.245401 ↗
14. 10.1103/PhysRevLett.116.13390310.1103/PhysRevLett.116.133903 ↗
15. 10.1103/PhysRevLett.121.02680810.1103/PhysRevLett.121.026808 ↗
16. 10.1103/PhysRevLett.124.05680210.1103/PhysRevLett.124.056802 ↗
17. 10.1103/PhysRevLett.123.24680110.1103/PhysRevLett.123.246801 ↗
18. 10.1126/science.aaz872710.1126/science.aaz8727 ↗
19. 10.1103/PhysRevLett.132.11380210.1103/PhysRevLett.132.113802 ↗
20. 10.34133/2021/560803810.34133/2021/5608038 ↗
21. 10.1038/s41567-020-0922-910.1038/s41567-020-0922-9 ↗
22. 10.1002/advs.20230112810.1002/advs.202301128 ↗
23. 10.1016/j.ymssp.2021.10877410.1016/j.ymssp.2021.108774 ↗
24. 10.1073/pnas.201058011710.1073/pnas.2010580117 ↗
25. 10.1038/s41567-020-0836-610.1038/s41567-020-0836-6 ↗
26. 10.1002/andp.20180002310.1002/andp.201800023 ↗
27. 10.1103/PhysRevLett.129.01390310.1103/PhysRevLett.129.013903 ↗
28. 10.1103/PhysRevLett.130.20360510.1103/PhysRevLett.130.203605 ↗
29. 10.1038/s41586-024-07174-w10.1038/s41586-024-07174-w ↗
30. 10.1103/PhysRevX.8.04103110.1103/PhysRevX.8.041031 ↗
31. 10.1038/s41467-024-47186-810.1038/s41467-024-47186-8 ↗
32. 10.1103/PhysRevB.110.03542410.1103/PhysRevB.110.035424 ↗
33. 10.1038/s41467-020-18917-410.1038/s41467-020-18917-4 ↗
34. 10.1103/PhysRevB.110.13431710.1103/PhysRevB.110.134317 ↗
35. 10.1103/PhysRevB.107.24510710.1103/PhysRevB.107.245107 ↗
36. 10.1103/PhysRevB.105.19540710.1103/PhysRevB.105.195407 ↗
37. 10.1103/PhysRevB.103.07544110.1103/PhysRevB.103.075441 ↗
38. 10.1103/PhysRevB.102.04111910.1103/PhysRevB.102.041119 ↗
39. 10.1103/PhysRevB.103.07512610.1103/PhysRevB.103.075126 ↗
40. 10.1088/1361-648X/ad359310.1088/1361-648X/ad3593 ↗
41. 10.1103/PhysRevB.99.08130210.1103/PhysRevB.99.081302 ↗
42. 10.1103/PhysRevLett.121.13680210.1103/PhysRevLett.121.136802 ↗
43. 10.1103/PhysRevA.103.L04020210.1103/PhysRevA.103.L040202 ↗
44. 10.1103/PhysRevX.11.03101510.1103/PhysRevX.11.031015 ↗
45. 10.1002/andp.20230032110.1002/andp.202300321 ↗
46. 10.1103/PhysRevB.110.20542910.1103/PhysRevB.110.205429 ↗
47. 10.1103/PhysRevB.109.11511510.1103/PhysRevB.109.115115 ↗
48. 10.1103/PhysRevResearch.4.02308910.1103/PhysRevResearch.4.023089 ↗
49. 10.1364/AOP.52928910.1364/AOP.529289 ↗
50. 10.1103/PhysRevX.9.04101510.1103/PhysRevX.9.041015 ↗
51. J. K. Asbóth · 201610.1007/978-3-319-25607-8 ↗
52. 10.1103/PhysRevA.98.05211610.1103/PhysRevA.98.052116 ↗
53. 10.1103/PhysRevLett.125.12640210.1103/PhysRevLett.125.126402 ↗
54. 10.1103/PhysRevResearch.1.02301310.1103/PhysRevResearch.1.023013 ↗
55. 10.1103/PhysRevB.110.L12140110.1103/PhysRevB.110.L121401 ↗
56. 10.1103/PhysRevB.106.19542510.1103/PhysRevB.106.195425 ↗
57. 10.1103/PhysRevLett.126.01040110.1103/PhysRevLett.126.010401 ↗
58. 10.1103/PhysRevB.101.20541710.1103/PhysRevB.101.205417 ↗
59. 10.1103/PhysRevB.103.15512910.1103/PhysRevB.103.155129 ↗
60. 10.1103/PhysRevB.100.16543010.1103/PhysRevB.100.165430 ↗
61. 10.1103/PhysRevB.107.11541210.1103/PhysRevB.107.115412 ↗
62. 10.1103/PhysRevLett.124.08680110.1103/PhysRevLett.124.086801 ↗
63. 10.1103/PhysRevB.97.04510610.1103/PhysRevB.97.045106 ↗
64. 10.1103/PhysRevLett.42.169810.1103/PhysRevLett.42.1698 ↗
65. 10.1088/1367-2630/ac38ce10.1088/1367-2630/ac38ce ↗
66. 10.1103/PhysRevB.109.04541410.1103/PhysRevB.109.045414 ↗
67. 10.1016/j.cjph.2020.12.02510.1016/j.cjph.2020.12.025 ↗
68. 10.1103/PhysRevLett.83.263610.1103/PhysRevLett.83.2636 ↗
69. 10.1103/PhysRevB.108.08542510.1103/PhysRevB.108.085425 ↗
70. 10.1103/PhysRevB.99.08110310.1103/PhysRevB.99.081103 ↗
71. 10.1103/PhysRevA.110.01220910.1103/PhysRevA.110.012209 ↗
72. R. Cavalieri · 201610.1017/CBO9781316569252 ↗