Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Letter
  • Open Access

Non-Hermiticity induces localization: Good and bad resonances in power-law random banded matrices

Giuseppe De Tomasi1 and Ivan M. Khaymovich2,3

  • 1Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801-3080, USA
  • 2Nordita, Stockholm University and KTH Royal Institute of Technology, Hannes Alfvéns väg 12, SE-106 91 Stockholm, Sweden
  • 3Institute for Physics of Microstructures, Russian Academy of Sciences, 603950 Nizhny Novgorod, GSP-105, Russia

Phys. Rev. B 108, L180202 – Published 30 November, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L180202

Abstract

The power-law random banded matrix (PLRBM) is a paradigmatic ensemble to study the Anderson localization transition (AT). In d dimensions, the PLRBMs are random matrices with algebraic decaying off-diagonal elements Hnm∼1/|n−m|α, having AT at α=d. In this work, we investigate the fate of the PLRBM to non-Hermiticity (nH). We consider the case where the random on-site diagonal potential takes complex values, mimicking an open system, subject to random gain-loss terms. We understand the model analytically by generalizing the Anderson-Levitov resonance counting technique to the nH case. We identify two competing mechanisms due to nH: favoring localization and delocalization. The competition between the two gives rise to AT at d/2≤α≤d. The value of the critical α depends on the strength of the on-site potential, like in Hermitian disordered short-range models in d>2. Within the localized phase, the wave functions are algebraically localized with an exponent α even for α<d. This result provides an example of non-Hermiticity-induced localization and finds immediate application in phase transitions driven by weak measurements.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (61)

  1. T. Tao, Topics in Random Matrix Theory, Graduate Studies in Mathematics Vol. 132 (American Mathematical Society, Los Angeles, CA, 2011).
  2. M. Mehta, Random Matrices (Elsevier Science, New York, 2004).
  3. C. W. J. Beenakker, Random-matrix theory of quantum transport, Rev. Mod. Phys. 69, 731 (1997).
  4. F. Haake, Quantum Signatures of Chaos, Physics and Astronomy Online Library (Springer, New York, 2001).
  5. P. W. Anderson, Absence of diffusion in certain random lattices, Phys. Rev. 109, 1492 (1958).
  6. F. Evers and A. D. Mirlin, Anderson transitions, Rev. Mod. Phys. 80, 1355 (2008).
  7. A. D. Mirlin, Statistics of energy levels and eigenfunctions in disordered systems, Phys. Rep. 326, 259 (2000).
  8. A. D. Mirlin, Y. V. Fyodorov, F.-M. Dittes, J. Quezada, and T. H. Seligman, Transition from localized to extended eigenstates in the ensemble of power-law random banded matrices, Phys. Rev. E 54, 3221 (1996).
  9. Y. V. Fyodorov, A. Ossipov, and A. Rodriguez, The Anderson localization transition and eigenfunction multifractality in an ensemble of ultrametric random matrices, J. Stat. Mech.: Theory Exp. (2009) L12001.
  10. L. S. Levitov, Absence of localization of vibrational modes due to dipole-dipole interaction, Europhys. Lett. 9, 83 (1989).
  11. L. S. Levitov, Delocalization of vibrational modes caused by electric dipole interaction, Phys. Rev. Lett. 64, 547 (1990).
  12. J. Šuntajs, M. Hopjan, W. D. Roeck, and L. Vidmar, Similarity between a many-body quantum avalanche model and the ultrametric random matrix model, arXiv:2308.07431.
  13. Note that the skin effect, denoted as nH, has no relation to Anderson localization observed in transport phenomena. In Anderson localization, the left and right eigenvectors localize at opposite ends of the sample. At the same time, the transport properties are dictated by the overlap of these vectors' envelopes, which may still exhibit delocalization.
  14. D. S. Borgnia, A. J. Kruchkov, and R.-J. Slager, Non-Hermitian boundary modes and topology, Phys. Rev. Lett. 124, 056802 (2020).
  15. N. Okuma, K. Kawabata, K. Shiozaki, and M. Sato, Topological origin of non-Hermitian skin effects, Phys. Rev. Lett. 124, 086801 (2020).
  16. S. Yao and Z. Wang, Edge states and topological invariants of non-Hermitian systems, Phys. Rev. Lett. 121, 086803 (2018).
  17. M. S. Rudner and L. S. Levitov, Topological transition in a non-Hermitian quantum walk, Phys. Rev. Lett. 102, 065703 (2009).
  18. Y. C. Hu and T. L. Hughes, Absence of topological insulator phases in non-Hermitian PT-symmetric Hamiltonians, Phys. Rev. B 84, 153101 (2011).
  19. K. Esaki, M. Sato, K. Hasebe, and M. Kohmoto, Edge states and topological phases in non-Hermitian systems, Phys. Rev. B 84, 205128 (2011).
  20. Z. Gong, Y. Ashida, K. Kawabata, K. Takasan, S. Higashikawa, and M. Ueda, Topological phases of non-Hermitian systems, Phys. Rev. X 8, 031079 (2018).
  21. H. Schomerus, Topologically protected midgap states in complex photonic lattices, Opt. Lett. 38, 1912 (2013).
  22. Y. Ashida, Z. Gong, and M. Ueda, Non-Hermitian physics, Adv. Phys. 69, 249 (2020).
  23. N. Moiseyev, Non-Hermitian Quantum Mechanics (Cambridge University Press, Cambridge, 2011).
  24. B. Skinner, J. Ruhman, and A. Nahum, Measurement-induced phase transitions in the dynamics of entanglement, Phys. Rev. X 9, 031009 (2019).
  25. A. Zabalo, M. J. Gullans, J. H. Wilson, R. Vasseur, A. W. W. Ludwig, S. Gopalakrishnan, D. A. Huse, and J. H. Pixley, Operator scaling dimensions and multifractality at measurement-induced transitions, Phys. Rev. Lett. 128, 050602 (2022).
  26. J. Feinberg and A. Zee, Non-Hermitian localization and delocalization, Phys. Rev. E 59, 6433 (1999).
  27. L. G. Molinari, Non-Hermitian spectra and Anderson localization, J. Phys. A: Math. Theor. 42, 265204 (2009).
  28. Y. Huang and B. I. Shklovskii, Anderson transition in three-dimensional systems with non-Hermitian disorder, Phys. Rev. B 101, 014204 (2020).
  29. Y. Huang and B. I. Shklovskii, Spectral rigidity of non-Hermitian symmetric random matrices near the Anderson transition, Phys. Rev. B 102, 064212 (2020).
  30. K. Kawabata and S. Ryu, Nonunitary scaling theory of non-Hermitian localization, Phys. Rev. Lett. 126, 166801 (2021).
  31. E. J. Bergholtz, J. C. Budich, and F. K. Kunst, Exceptional topology of non-Hermitian systems, Rev. Mod. Phys. 93, 015005 (2021).
  32. Y. Li, X. Chen, and M. P. A. Fisher, Quantum Zeno effect and the many-body entanglement transition, Phys. Rev. B 98, 205136 (2018).
  33. A. Chan, R. M. Nandkishore, M. Pretko, and G. Smith, Unitary-projective entanglement dynamics, Phys. Rev. B 99, 224307 (2019).
  34. N. Hatano and D. R. Nelson, Localization transitions in non-Hermitian quantum mechanics, Phys. Rev. Lett. 77, 570 (1996).
  35. D. Bernard and A. LeClair, A classification of non-Hermitian random matrices, in Statistical Field Theories, edited by A. Cappelli and G. Mussardo (Springer Netherlands, Dordrecht, 2002), pp. 207–214.
  36. X. Luo, T. Ohtsuki, and R. Shindou, Universality classes of the Anderson transitions driven by non-Hermitian disorder, Phys. Rev. Lett. 126, 090402 (2021).
  37. X. Luo, Z. Xiao, K. Kawabata, T. Ohtsuki, and R. Shindou, Unifying the Anderson transitions in Hermitian and non-Hermitian systems, Phys. Rev. Res. 4, L022035 (2022).
  38. R. Hamazaki, K. Kawabata, and M. Ueda, Non-Hermitian many-body localization, Phys. Rev. Lett. 123, 090603 (2019).
  39. A. F. Tzortzakakis, K. G. Makris, and E. N. Economou, Non-Hermitian disorder in two-dimensional optical lattices, Phys. Rev. B 101, 014202 (2020).
  40. A. F. Tzortzakakis, K. G. Makris, A. Szameit, and E. N. Economou, Transport and spectral features in non-Hermitian open systems, Phys. Rev. Res. 3, 013208 (2021).
  41. G. De Tomasi and I. M. Khaymovich, Non-Hermitian Rosenzweig-Porter random-matrix ensemble: Obstruction to the fractal phase, Phys. Rev. B 106, 094204 (2022).
  42. G. D. Tomasi and I. M. Khaymovich, Stable many-body localization under random continuous measurements in the no-click limit, arXiv:2311.00019.
  43. E. Granet, C. Zhang, and H. Dreyer, Volume-law to area-law entanglement transition in a nonunitary periodic Gaussian circuit, Phys. Rev. Lett. 130, 230401 (2023).
  44. H. Burau, M. Heyl, and G. De Tomasi, Fate of algebraic many-body localization under driving, Phys. Rev. B 104, 224201 (2021).
  45. δR is given by the ratio of the width of the on-site random potential −W/2<ɛm<W/2 to the number ∼Rd of lattice sites in the ring (4).
  46. For the exact definitions and expressions of both probabilities see the Supplemental Material [47].
  47. See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevB.108.L180202 for details of calculations of the probabilities of resonances; which includes Ref. [11].
  48. J. Ginibre, Statistical ensembles of complex, quaternion, and real matrices, J. Math. Phys. 6, 440 (1965).
  49. L. Sá, P. Ribeiro, and T. Prosen, Complex spacing ratios: A signature of dissipative quantum chaos, Phys. Rev. X 10, 021019 (2020).
  50. We have checked in the Supplemental Materials [47] that IPR is statistically the same for left eigenvectors and mixed definitions IPRqr=∑m|ψnr(m)ψnl(m)|q.
  51. X. Deng, V. E. Kravtsov, G. V. Shlyapnikov, and L. Santos, Duality in power-law localization in disordered one-dimensional systems, Phys. Rev. Lett. 120, 110602 (2018).
  52. P. A. Nosov, I. M. Khaymovich, and V. E. Kravtsov, Correlation-induced localization, Phys. Rev. B 99, 104203 (2019).
  53. P. A. Nosov and I. M. Khaymovich, Robustness of delocalization to the inclusion of soft constraints in long-range random models, Phys. Rev. B 99, 224208 (2019).
  54. X. Deng, A. L. Burin, and I. M. Khaymovich, Anisotropy-mediated reentrant localization, SciPost Phys. 13, 116 (2022).
  55. A. G. Kutlin and I. M. Khaymovich, Renormalization to localization without a small parameter, SciPost Phys. 8, 049 (2020).
  56. V. R. Motamarri, A. S. Gorsky, and I. M. Khaymovich, Localization and fractality in disordered Russian Doll model, SciPost Phys. 13, 117 (2022).
  57. W. Tang and I. M. Khaymovich, Non-ergodic delocalized phase with Poisson level statistics, Quantum 6, 733 (2022).
  58. K. Jacobs and D. A. Steck, A straightforward introduction to continuous quantum measurement, Contemp. Phys. 47, 279 (2006).
  59. H. M. Wiseman and G. J. Milburn, Quantum Measurement and Control (Cambridge University Press, Cambridge, 2009).
  60. X. Turkeshi, A. Biella, R. Fazio, M. Dalmonte, and M. Schiró, Measurement-induced entanglement transitions in the quantum Ising chain: From infinite to zero clicks, Phys. Rev. B 103, 224210 (2021).
  61. X. Turkeshi and M. Schiró, Entanglement and correlation spreading in non-Hermitian spin chains, Phys. Rev. B 107, L020403 (2023).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation