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arxiv: 2603.25451 · v3 · submitted 2026-03-26 · ⚛️ physics.optics · quant-ph

Exceptional-point-constrained locking of boundary-sensitive topological transitions in chiral non-Hermitian SSH-type lattices

Pith reviewed 2026-05-15 06:50 UTC · model grok-4.3

classification ⚛️ physics.optics quant-ph
keywords non-Hermitian topologyexceptional pointsSSH latticepoint-gap windingnon-Bloch bandsboundary modeschiral symmetrytopological transitions
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The pith

EP-constrained sweeps lock PBC and OBC topological transitions in non-Hermitian SSH lattices

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

In non-Hermitian systems topological transitions under periodic and open boundary conditions are generally governed by different spectra and therefore do not coincide. This paper shows that in a class of chiral non-Hermitian SSH-type lattices, parameter paths that keep a zero-energy Bloch degeneracy present throughout the sweep force the two transitions to occur at the same point. The persistence of this degeneracy, which is exceptional in the non-Hermitian setting, produces the locking: a change in point-gap winding under periodic boundaries now marks the non-Bloch real-line-gap transition under open boundaries and the associated change in zero-energy boundary modes. Closed-form results are given for an extended two-band chain, while generalized Brillouin-zone numerics confirm the effect in generic two-band and four-band cases; unconstrained paths lack the locking.

Core claim

For chiral non-Hermitian Su-Schrieffer-Heeger type lattices, exceptional-point-constrained parameter evolutions lock the point-gap winding transition under periodic boundary conditions to the non-Bloch bulk real-line-gap transition under open boundary conditions at Re(E)=0. The locking holds because the zero-energy Bloch degeneracy persists along the entire sweep. In an analytically tractable limit the EP-constrained manifolds and both transition boundaries are obtained in closed form; away from the limit, generalized-Brillouin-zone calculations verify the correspondence for representative constrained sweeps while showing that isolated exceptional points or Hermitian degeneracies do not lock

What carries the argument

Exceptional-point-constrained parameter evolution that preserves a zero-energy Bloch degeneracy along the entire sweep

Load-bearing premise

A zero-energy Bloch degeneracy persists along the full parameter sweep in the non-Hermitian regime

What would settle it

A numerical sweep that maintains the zero-energy degeneracy throughout yet shows a PBC winding change without a corresponding OBC real-line-gap transition at Re(E)=0

read the original abstract

Topological transitions in non-Hermitian systems are generally boundary sensitive: a point-gap winding transition under periodic boundary condition (PBC) and a non-Bloch bulk real-line-gap transition under open boundary condition (OBC) at $\mathrm{Re}(E)=0$ are governed by different spectra and therefore need not coincide. Here we show, for a class of chiral non-Hermitian Su--Schrieffer--Heeger (SSH)-type lattices, that these two criticalities can be locked by an exceptional-point-constrained (EP-constrained) parameter evolution. The key requirement is not the occurrence of isolated exceptional points, but the persistence of a zero-energy Bloch degeneracy along the entire sweep, which is generically exceptional in the non-Hermitian regime. In an analytically tractable limit of an extended non-Hermitian SSH chain, the EP-constrained manifolds and both transition boundaries are obtained in closed form, making the locking explicit. Away from this limit, numerical generalized-Brillouin-zone (GBZ) calculations confirm the correspondence for representative constrained sweeps, whereas unconstrained paths show that isolated exceptional points or Hermitian degeneracies do not enforce locking. We further verify the mechanism in a spinful four-band extension with branch-resolved GBZs, including strongly branch-imbalanced regimes. These results establish a path-dependent diagnostic principle: along EP-constrained sweeps in this SSH-type class, changes in PBC point-gap winding can indicate OBC non-Bloch bulk real-line-gap transitions and the corresponding changes in zero-energy boundary modes.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 3 minor

Summary. The manuscript claims that in chiral non-Hermitian SSH-type lattices, exceptional-point-constrained parameter sweeps lock PBC point-gap winding transitions to OBC non-Bloch real-line-gap transitions (and associated zero-mode changes) at Re(E)=0. This locking occurs because a zero-energy Bloch degeneracy persists along the entire sweep. Closed-form expressions for the EP-constrained manifolds and both transition boundaries are derived in an analytically tractable limit of an extended non-Hermitian SSH chain; GBZ numerics confirm the correspondence for representative constrained paths (with counter-examples for unconstrained paths) and extend to a spinful four-band model with branch-resolved GBZs.

Significance. If the central claim holds, the work supplies a concrete path-dependent diagnostic that connects PBC winding changes to OBC non-Bloch bulk transitions in this SSH class, with the persistence of the zero-energy degeneracy as the enabling mechanism. The closed-form results in the tractable limit and the reproducible GBZ checks constitute clear strengths that allow direct verification of the locking without fitted parameters.

major comments (1)
  1. [Analytically tractable limit] The central locking mechanism rests on persistence of the zero-energy Bloch degeneracy along the full EP-constrained path. While the abstract states this requirement explicitly and the tractable-limit derivation obtains the manifolds in closed form, the manuscript should add an explicit verification (perhaps as a short lemma or appendix) that the degeneracy condition is identically satisfied on the derived manifolds rather than imposed separately.
minor comments (3)
  1. [Numerical verification] The GBZ plots for the four-band extension would benefit from explicit labeling of the branch-resolved spectra and a brief statement of the numerical tolerance used to identify the real-line gap closing.
  2. [Introduction] The counter-examples for unconstrained paths are mentioned but not cross-referenced to specific parameter values or figures; adding one or two explicit unconstrained trajectories alongside the constrained ones would make the contrast immediate.
  3. Notation for the generalized Brillouin zone and the point-gap winding number should be defined once in a dedicated paragraph before the first use to avoid ambiguity in the multi-band extension.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the positive assessment and the constructive suggestion regarding the analytically tractable limit. We address the comment below.

read point-by-point responses
  1. Referee: [Analytically tractable limit] The central locking mechanism rests on persistence of the zero-energy Bloch degeneracy along the full EP-constrained path. While the abstract states this requirement explicitly and the tractable-limit derivation obtains the manifolds in closed form, the manuscript should add an explicit verification (perhaps as a short lemma or appendix) that the degeneracy condition is identically satisfied on the derived manifolds rather than imposed separately.

    Authors: We agree that an explicit verification would strengthen the presentation of the locking mechanism. In the revised manuscript we add a short lemma in Appendix A. The lemma proves that the zero-energy Bloch degeneracy holds identically on the derived EP-constrained manifolds: it follows directly from the chiral symmetry of the extended non-Hermitian SSH Hamiltonian together with the closed-form expressions for the manifolds, without any separate imposition of the degeneracy condition. revision: yes

Circularity Check

0 steps flagged

No significant circularity; closed-form derivation stands independently

full rationale

The central claim is established by explicit closed-form solution of the EP-constrained manifolds and both transition boundaries in the analytically tractable extended non-Hermitian SSH limit. The persistence of the zero-energy Bloch degeneracy is introduced as an explicit necessary condition and used directly to derive the locking; it is not obtained by fitting, self-definition, or prior self-citation. GBZ numerics are presented only as confirmation for representative paths and counter-examples, not as the source of the result. No load-bearing step reduces to its own input by construction, and no uniqueness theorem or ansatz is imported via self-citation.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The claim rests on standard non-Hermitian band theory and GBZ formalism plus the new requirement of persistent zero-energy degeneracy; no new particles or forces are introduced.

free parameters (1)
  • hopping amplitudes in the extended non-Hermitian SSH chain
    Model parameters swept along the constrained paths; their specific values define the analytically tractable limit.
axioms (1)
  • domain assumption Generalized Brillouin zone formalism accurately captures OBC spectra in non-Hermitian lattices
    Invoked for all numerical verification of the locking.

pith-pipeline@v0.9.0 · 5587 in / 1302 out tokens · 43439 ms · 2026-05-15T06:50:07.412351+00:00 · methodology

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Reference graph

Works this paper leans on

68 extracted references · 68 canonical work pages

  1. [1]

    Bender, C. M. & Boettcher, S. Real spectra in non-Hermitian ha miltonians having PT symmetry. Phys. Rev. Lett. 80, 5243–5246 (1998)

  2. [2]

    Shen, H., Zhen, B. & Fu, L. Topological band theory for non-Her mitian hamiltonians. Phys. Rev. Lett. 120, 146402 (2018)

  3. [3]

    J., Budich, J

    Bergholtz, E. J., Budich, J. C. & Kunst, F. K. Exceptional topolo gy of non- Hermitian systems. Rev. Mod. Phys. 93, 015005 (2021)

  4. [4]

    & Ueda, M

    Ashida, Y., Gong, Z. & Ueda, M. Non-Hermitian physics. Adv. Phys. 69, 249–435 (2020). 19

  5. [5]

    Schreiber, A. et al. Decoherence and disorder in quantum walks: From ballistic spread to localization. Phys. Rev. Lett. 106, 180403 (2011)

  6. [6]

    Liang, Q. et al. Dynamic signatures of non-Hermitian skin effect and topology in ultracold atoms. Phys. Rev. Lett. 129, 070401 (2022)

  7. [7]

    & Schomerus, H

    Poli, C., Bellec, M., Kuhl, U., Mortessagne, F. & Schomerus, H. Selec tive enhance- ment of topologically induced interface states in a dielectric resonat or chain. Nat. Commun. 6, 6710 (2015)

  8. [8]

    Bandres, M. A. et al. Topological insulator laser: Experiments. Science 359, eaar4005 (2018)

  9. [9]

    Parto, M. et al. Edge-mode lasing in 1D topological active arrays. Phys. Rev. Lett. 120, 113901 (2018)

  10. [10]

    Xiao, L. et al. Observation of topological edge states in parity–time-symmetric quantum walks. Nat. Phys. 13, 1117–1123 (2017)

  11. [11]

    & Xue, P

    Xiao, L., Sarkar, S., Wang, K., Bayat, A. & Xue, P. Observation o f criticality- enhanced quantum sensing in nonunitary quantum walks. Phys. Rev. Lett. 136, 060802 (2026)

  12. [12]

    & Lee, C

    Lin, R., Tai, T., Li, L. & Lee, C. H. Topological non-Hermitian skin eff ect. Front. Phys. 18, 53605 (2023)

  13. [13]

    S., Kruchkov, A

    Borgnia, D. S., Kruchkov, A. J. & Slager, R. J. Non-Hermitian bo undary modes and topology. Phys. Rev. Lett. 124, 056802 (2020)

  14. [14]

    Lee, C. H. & Thomale, R. Anatomy of skin modes and topology in no n-Hermitian systems. Phys. Rev. B 99, 201103 (2019)

  15. [15]

    Li, L., Lee, C. H. & Gong, J. Geometric characterization of non- Hermitian topo- logical systems through the singularity ring in pseudospin vector sp ace. Phys. Rev. B 100, 075403 (2019)

  16. [16]

    & Sato, M

    Okuma, N., Kawabata, K., Shiozaki, K. & Sato, M. Topological orig in of non- Hermitian skin effects. Phys. Rev. Lett. 124, 086801 (2020)

  17. [17]

    Gong, Z. et al. Topological phases of non-Hermitian systems. Phys. Rev. X 8, 031079 (2018)

  18. [18]

    & Fang, C

    Zhang, K., Yang, Z. & Fang, C. Correspondence between windin g numbers and skin modes in non-Hermitian systems. Phys. Rev. Lett. 125, 126402 (2020)

  19. [19]

    & Ryu, S

    Kawabata, K., Numasawa, T. & Ryu, S. Entanglement phase tra nsition induced by the non-Hermitian skin effect. Phys. Rev. X 13, 021007 (2023). 20

  20. [20]

    Lee, T. E. Anomalous edge state in a non-Hermitian lattice. Phys. Rev. Lett. 116, 133903 (2016)

  21. [21]

    H., Li, L

    Lee, C. H., Li, L. & Gong, J. Hybrid higher-order skin-topologica l modes in nonreciprocal systems. Phys. Rev. Lett. 123, 016805 (2019)

  22. [22]

    & Barci, D

    Aquino, R., Lopes, N. & Barci, D. G. Critical and noncritical non- Hermitian topological phase transitions in one-dimensional chains. Phys. Rev. B 107, 035424 (2023)

  23. [23]

    K., Edvardsson, E., Budich, J

    Kunst, F. K., Edvardsson, E., Budich, J. C. & Bergholtz, E. J. B iorthogonal bulk-boundary correspondence in non-Hermitian systems. Phys. Rev. Lett. 121, 026808 (2018)

  24. [24]

    & Yang, Z

    Yi, Y. & Yang, Z. Non-Hermitian skin modes induced by on-site diss ipations and chiral tunneling effect. Phys. Rev. Lett. 125, 186802 (2020)

  25. [25]

    & Wang, Z

    Song, F., Yao, S. & Wang, Z. Non-Hermitian topological invariant s in real space. Phys. Rev. Lett. 123, 246801 (2019)

  26. [26]

    Self-healing of non-Hermitian topological skin modes

    Longhi, S. Self-healing of non-Hermitian topological skin modes. Phys. Rev. Lett. 128, 157601 (2022)

  27. [27]

    & Sato, M

    Kawabata, K., Shiozaki, K., Ueda, M. & Sato, M. Symmetry and to pology in non-Hermitian physics. Phys. Rev. X 9, 041015 (2019)

  28. [28]

    Yang, Z., Zhang, K., Fang, C. & Hu, J. Non-Hermitian bulk-bound ary corre- spondence and auxiliary generalized Brillouin zone theory. Phys. Rev. Lett. 125, 226402 (2020)

  29. [29]

    & Sato, M

    Nakamura, D., Bessho, T. & Sato, M. Bulk-boundary correspo ndence in point-gap topological phases. Phys. Rev. Lett. 132, 136401 (2024)

  30. [30]

    Li, Y., Li, L. & Xu, Z. Size-dependent skin effect transitions in wea kly coupled nonreciprocal chains. Phys. Rev. B 112, 235122 (2025)

  31. [31]

    & Wang, Z

    Yao, S. & Wang, Z. Edge states and topological invariants of no n-Hermitian systems. Phys. Rev. Lett. 121, 086803 (2018)

  32. [32]

    & Wang, Z

    Yao, S., Song, F. & Wang, Z. Non-Hermitian Chern bands. Phys. Rev. Lett. 121, 136802 (2018)

  33. [33]

    & Murakami, S

    Yokomizo, K. & Murakami, S. Non-Bloch band theory of non-Her mitian systems. Phys. Rev. Lett. 123, 066404 (2019)

  34. [34]

    & Murakami, S

    Yokomizo, K. & Murakami, S. Non-Bloch band theory and bulk–ed ge corre- spondence in non-Hermitian systems. Prog. Theor. Exp. Phys. 2020, 12A102 (2020). 21

  35. [35]

    Xu, K. et al. Coexistence of topological edge states and skin effects in the non- Hermitian Su-Schrieffer-Heeger model with long-range nonrecipro cal hopping in topoelectric realizations. Phys. Rev. B 103, 125411 (2021)

  36. [36]

    & Bergholtz, E

    Yang, F. & Bergholtz, E. J. Anatomy of higher-order non-Her mitian skin and boundary modes. Phys. Rev. Res. 7, 023233 (2025)

  37. [37]

    & Kawabata, K

    Hamanaka, S., Yoshida, T. & Kawabata, K. Non-Hermitian topolo gy in Hermitian topological matter. Phys. Rev. Lett. 133, 266604 (2024)

  38. [38]

    & L¨ u, X.-Y

    Wan, L.-L. & L¨ u, X.-Y. Quantum-squeezing-induced point-gap topology and skin effect. Phys. Rev. Lett. 130, 203605 (2023)

  39. [39]

    & Kawabata, K

    Schindler, F., Gu, K., Lian, B. & Kawabata, K. Hermitian bulk – non- Hermitian boundary correspondence. PRX Quantum 4, 030315 (2023)

  40. [40]

    Liu, D. et al. Simultaneous manipulation of line-gap and point-gap topologies in non-Hermitian lattices. Laser Photonics Rev. 17, 2200371 (2023)

  41. [41]

    & Lee, C

    Qin, F., Ma, Y., Shen, R. & Lee, C. H. Universal competitive spect ral scaling from the critical non-Hermitian skin effect. Phys. Rev. B 107, 155430 (2023)

  42. [42]

    Helbig, T. et al. Generalized bulk–boundary correspondence in non-Hermitian topolectrical circuits. Nat. Phys. 16, 747–750 (2020)

  43. [43]

    Xiao, L. et al. Non-Hermitian bulk–boundary correspondence in quantum dynamics. Nat. Phys. 16, 761–766 (2020)

  44. [44]

    Weidemann, S. et al. Topological funneling of light. Science 368, 311–314 (2020)

  45. [45]

    Xiao, L. et al. Observation of non-Bloch parity-time symmetry and exceptional points. Phys. Rev. Lett. 126, 230402 (2021)

  46. [46]

    Heiss, W. D. Exceptional points of non-Hermitian operators. J. Phys. A: Math. Gen. 37, 2455–2464 (2004)

  47. [47]

    Miri, M. A. & Alu, A. Exceptional points in optics and photonics. Science 363, eaar7709 (2019)

  48. [48]

    Chen, H. Z. et al. Revealing the missing dimension at an exceptional point. Nat. Phys. 16, 571–578 (2020)

  49. [49]

    Dembowski, C. et al. Encircling an exceptional point. Phys. Rev. E 69, 056216 (2004)

  50. [50]

    Doppler, J. et al. Dynamically encircling an exceptional point for asymmetric mode switching. Nature 537, 76–79 (2016). 22

  51. [51]

    P., Schrieffer, J

    Su, W. P., Schrieffer, J. R. & Heeger, A. J. Solitons in polyacetyle ne. Phys. Rev. Lett. 42, 1698–1701 (1979)

  52. [52]

    Probing non-Hermitian skin effect and non-Bloch phas e transitions

    Longhi, S. Probing non-Hermitian skin effect and non-Bloch phas e transitions. Phys. Rev. Res. 1, 023013 (2019)

  53. [53]

    Lin, R. & Li, L. Topologically compatible non-Hermitian skin effect. Phys. Rev. B 109, 155137 (2024)

  54. [54]

    & Zhang, Y

    Xu, Z., Zhang, R., Chen, S., Fu, L. & Zhang, Y. Fate of zero mode s in a finite Su-Schrieffer-Heeger model with PT symmetry. Phys. Rev. A 101, 013635 (2020)

  55. [55]

    M., Siu, Z

    Rafi-Ul-Islam, S. M., Siu, Z. B., Sahin, H., Lee, C. H. & Jalil, M. B. A. C ritical hybridization of skin modes in coupled non-Hermitian chains. Phys. Rev. Res. 4, 013243 (2022)

  56. [56]

    M., Siu, Z

    Rafi-Ul-Islam, S. M., Siu, Z. B., Razo, M. S. H. & Jalil, M. B. A. Critica l non- Hermitian skin effect in a cross-coupled Hermitian chain. Phys. Rev. B 111, 115415 (2025)

  57. [57]

    Li, L., Lee, C. H. & Gong, J. Topological switch for non-Hermitian skin effect in cold-atom systems with loss. Phys. Rev. Lett. 124, 250402 (2020)

  58. [58]

    Zhao, E. et al. Two-dimensional non-Hermitian skin effect in an ultracold Fermi gas. Nature 637, 565–573 (2025)

  59. [59]

    Wang, H., Xu, Z. & Li, Z. Topological phase transitions and edge- state transfer in time-multiplexed quantum walks. Phys. Rev. A 112, 042230 (2025)

  60. [60]

    Li, L., Lee, C. H. & Gong, J. Impurity induced scale-free localizat ion. Commun. Phys. 4, 42 (2021)

  61. [61]

    Liu, J. & Xu, Z. From ergodicity to many-body localization in a one- dimensional interacting non-Hermitian Stark system. Phys. Rev. B 108, 184205 (2023)

  62. [62]

    & Chen, S

    Xu, Z. & Chen, S. Topological Bose-Mott insulators in one-dimen sional non- Hermitian superlattices. Phys. Rev. B 102, 035153 (2020)

  63. [63]

    S., Lee, C

    Qin, Y., Ang, Y. S., Lee, C. H. & Li, L. Many-body critical non-Her mitian skin effect. Commun. Phys. 9, 16 (2026)

  64. [64]

    Liu, S. et al. Non-Hermitian entanglement dip from scaling-induced exceptional criticality. Sci. Bull. 70, 2929–2932 (2025)

  65. [65]

    & Lee, C

    Yang, M. & Lee, C. H. Percolation-induced PT symmetry breakin g. Phys. Rev. Lett. 133, 136602 (2024). 23

  66. [66]

    Wang, K. et al. Generating arbitrary topological windings of a non-Hermitian band. Science 371, 1240–1245 (2021)

  67. [67]

    Park, J. et al. Revealing non-Hermitian band structure of photonic Floquet media. Sci. Adv. 8, eabo6220 (2022)

  68. [68]

    Cao, M. M. et al. Probing complex-energy topology via non-Hermitian absorption spectroscopy in a trapped ion simulator. Phys. Rev. Lett. 130, 163001 (2023). Acknowledgements Z. X. acknowledges support from National Natural Science Found ation of China (Grants No. 12375016 and No. 12461160324) and Beijing National Laboratory for Condensed Matter Physics (G...