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
  • Open Access

Anomalous multigap topological phases in periodically driven quantum rotors

Volker Karle1,*, Mikhail Lemeshko1,†, Adrien Bouhon2,3, Robert-Jan Slager2,4,‡, and F. Nur Ünal2,5,§

  • *Contact author: volker.karle@ista.ac.at
  • †Contact author: mikhail.lemeshko@ista.ac.at
  • ‡Contact author: rjs269@cam.ac.uk
  • §Contact author: fnu20@cam.ac.uk

Phys. Rev. A 113, 012216 – Published 12 January, 2026

DOI: https://doi.org/10.1103/db9d-9bns

Abstract

We demonstrate that periodically driven quantum rotors provide a promising and broadly applicable platform to implement multigap topological phases, where groups of bands can acquire topological invariants due to non-Abelian braiding of band degeneracies. By adiabatically varying the periodic kicks to the rotor we find nodal-line braiding, which causes sign flips of topological charges of band nodes and can prevent them from annihilating, indicated by nonzero values of the patch Euler class. In particular, we report on the emergence of an anomalous Dirac string phase arising in the strongly driven regime, a truly out-of-equilibrium phase of the quantum rotor. This phase emanates from braiding processes involving all (quasienergy) gaps and manifests itself with edge states at zero angular momentum. Our results reveal direct applications in state-of-the-art experiments of quantum rotors, such as linear molecules driven by periodic far-off-resonant laser pulses or artificial quantum rotors in optical lattices, whose extensive versatility offers precise modification and observation of novel non-Abelian topological properties.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (73)

  1. X.-L. Qi and S.-C. Zhang, Topological insulators and superconductors, Rev. Mod. Phys. 83, 1057 (2011).
  2. M. Z. Hasan and C. L. Kane, Colloquium: Topological insulators, Rev. Mod. Phys. 82, 3045 (2010).
  3. L. Fu, Topological crystalline insulators, Phys. Rev. Lett. 106, 106802 (2011).
  4. R.-J. Slager, A. Mesaros, V. Juričić, and J. Zaanen, The space group classification of topological band-insulators, Nat. Phys. 9, 98 (2013).
  5. J. Kruthoff, J. de Boer, J. van Wezel, C. L. Kane, and R.-J. Slager, Topological classification of crystalline insulators through band structure combinatorics, Phys. Rev. X 7, 041069 (2017).
  6. H. C. Po, A. Vishwanath, and H. Watanabe, Symmetry-based indicators of band topology in the 230 space groups, Nat. Commun. 8, 50 (2017).
  7. B. Bradlyn, L. Elcoro, J. Cano, M. G. Vergniory, Z. Wang, C. Felser, M. I. Aroyo, and B. A. Bernevig, Topological quantum chemistry, Nature (London) 547, 298 (2017).
  8. R.-J. Slager, The translational side of topological band insulators, J. Phys. Chem. Solids 128, 24 (2019), Spin-Orbit Coupled Materials.
  9. K. Shiozaki and M. Sato, Topology of crystalline insulators and superconductors, Phys. Rev. B 90, 165114 (2014).
  10. N. P. Armitage, E. J. Mele, and A. Vishwanath, Weyl and Dirac semimetals in three-dimensional solids, Rev. Mod. Phys. 90, 015001 (2018).
  11. T. Kitagawa, E. Berg, M. Rudner, and E. Demler, Topological characterization of periodically driven quantum systems, Phys. Rev. B 82, 235114 (2010).
  12. M. S. Rudner, N. H. Lindner, E. Berg, and M. Levin, Anomalous edge states and the bulk-edge correspondence for periodically driven two-dimensional systems, Phys. Rev. X 3, 031005 (2013).
  13. R. Roy and F. Harper, Periodic table for Floquet topological insulators, Phys. Rev. B 96, 155118 (2017).
  14. F. N. Ünal, A. Eckardt, and R.-J. Slager, Hopf characterization of two-dimensional Floquet topological insulators, Phys. Rev. Res. 1, 022003(R) (2019).
  15. J. Ahn, S. Park, and B.-J. Yang, Failure of Nielsen-Ninomiya theorem and fragile topology in two-dimensional systems with space-time inversion symmetry: Application to twisted bilayer graphene at magic angle, Phys. Rev. X 9, 021013 (2019).
  16. A. Bouhon, Q. Wu, R.-J. Slager, H. Weng, O. V. Yazyev, and T. Bzdušek, Non-Abelian reciprocal braiding of Weyl points and its manifestation in ZrTe, Nat. Phys. 16, 1137 (2020).
  17. A. Bouhon, T. Bzdusek, and R.-J. Slager, Geometric approach to fragile topology beyond symmetry indicators, Phys. Rev. B 102, 115135 (2020).
  18. A. Bouhon, A. M. Black-Schaffer, and R.-J. Slager, Wilson loop approach to fragile topology of split elementary band representations and topological crystalline insulators with time-reversal symmetry, Phys. Rev. B 100, 195135 (2019).
  19. W. J. Jankowski, A. S. Morris, Z. Davoyan, A. Bouhon, F. N. Ünal, and R.-J. Slager, Non-Abelian Hopf-Euler insulators, Phys. Rev. B 110, 075135 (2024).
  20. J. Ahn and B.-J. Yang, Symmetry representation approach to topological invariants in C2zT-symmetric systems, Phys. Rev. B 99, 235125 (2019).
  21. Z. Davoyan, W. J. Jankowski, A. Bouhon, and R.-J. Slager, Three-dimensional PT-symmetric topological phases with a Pontryagin index, Phys. Rev. B 109, 165125 (2024).
  22. H. Lim, S. Kim, and B.-J. Yang, Real Hopf insulator, Phys. Rev. B 108, 125101 (2023).
  23. Q. Wu, A. A. Soluyanov, and T. Bzdušek, Non-Abelian band topology in noninteracting metals, Science 365, 1273 (2019).
  24. B. Peng, A. Bouhon, B. Monserrat, and R.-J. Slager, Phonons as a platform for non-Abelian braiding and its manifestation in layered silicates, Nat. Commun. 13, 423 (2022).
  25. B. Peng, A. Bouhon, R.-J. Slager, and B. Monserrat, Multigap topology and non-Abelian braiding of phonons from first principles, Phys. Rev. B 105, 085115 (2022).
  26. V. Könye, A. Bouhon, I. C. Fulga, R.-J. Slager, J. van den Brink, and J. I. Facio, Chirality flip of Weyl nodes and its manifestation in strained MoTe2, Phys. Rev. Res. 3, L042017 (2021).
  27. S. Chen, A. Bouhon, R.-J. Slager, and B. Monserrat, Non-Abelian braiding of Weyl nodes via symmetry-constrained phase transitions, Phys. Rev. B 105, L081117 (2022).
  28. A. Bouhon, G. F. Lange, and R.-J. Slager, Topological correspondence between magnetic space group representations and subdimensions, Phys. Rev. B 103, 245127 (2021).
  29. S. H. Lee, Y. Qian, and B.-J. Yang, Euler band topology in spin-orbit coupled magnetic systems, Phys. Rev. B 111, 245127 (2025).
  30. B. Jiang, A. Bouhon, Z.-K. Lin, X. Zhou, B. Hou, F. Li, R.-J. Slager, and J.-H. Jiang, Experimental observation of non-Abelian topological acoustic semimetals and their phase transitions, Nat. Phys. 17, 1239 (2021).
  31. B. Jiang, A. Bouhon, S.-Q. Wu, Z.-L. Kong, Z.-K. Lin, R.-J. Slager, and J.-H. Jiang, Observation of an acoustic topological Euler insulator with meronic waves, Sci. Bull. 69, 1653 (2024).
  32. T. Jiang, Q. Guo, R.-Y. Zhang, Z.-Q. Zhang, B. Yang, and C. T. Chan, Four-band non-Abelian topological insulator and its experimental realization, Nat. Commun. 12, 6471 (2021).
  33. E. Yang, B. Yang, O. You, H.-C. Chan, P. Mao, Q. Guo, S. Ma, L. Xia, D. Fan, Y. Xiang, and S. Zhang, Observation of non-Abelian nodal links in photonics, Phys. Rev. Lett. 125, 033901 (2020).
  34. Y. Yang, B. Yang, G. Ma, J. Li, S. Zhang, and C. T. Chan, Non-Abelian physics in light and sound, Science 383, eadf9621 (2024).
  35. F. N. Ünal, A. Bouhon, and R.-J. Slager, Topological Euler class as a dynamical observable in optical lattices, Phys. Rev. Lett. 125, 053601 (2020).
  36. W. D. Zhao, Y. B. Yang, Y. Jiang, Z. C. Mao, W. X. Guo, L. Y. Qiu, G. X. Wang, L. Yao, L. He, Z. C. Zhou, Y. Xu, and L. M. Duan, Observation of topological Euler insulators with a trapped-ion quantum simulator, Commun. Phys. 5, 223 (2022).
  37. R.-J. Slager, A. Bouhon, and F. N. Ünal, Non-Abelian Floquet braiding and anomalous Dirac string phase in periodically driven systems, Nat. Commun. 15, 1144 (2024).
  38. T. Li and H. Hu, Floquet non-Abelian topological insulator and multifold bulk-edge correspondence, Nat. Commun. 14, 6418 (2023).
  39. R.-J. Slager, A. Bouhon, and F. N. Ünal, Comment on “Floquet non-Abelian topological insulator and multifold bulk-edge correspondence,” arXiv:2310.12782.
  40. O. Breach, R.-J. Slager, and F. N. Ünal, Interferometry of non-Abelian band singularities and Euler class topology, Phys. Rev. Lett. 133, 093404 (2024).
  41. J. Wang and J. Gong, Proposal of a cold-atom realization of quantum maps with Hofstadter's butterfly spectrum, Phys. Rev. A 77, 031405(R) (2008).
  42. D. Y. H. Ho and J. Gong, Quantized adiabatic transport in momentum space, Phys. Rev. Lett. 109, 010601 (2012).
  43. L. Zhou and J. Gong, Floquet topological phases in a spin-1/2 double kicked rotor, Phys. Rev. A 97, 063603 (2018).
  44. I. Dana, Topological properties of adiabatically varied Floquet systems, Phys. Rev. E 96, 022216 (2017).
  45. F. Izrailev and D. L. Shepelyanskii, Quantum resonance for a rotator in a nonlinear periodic field, Theor. Math. Phys. 43, 553 (1980).
  46. M. S. Santhanam, S. Paul, and J. B. Kannan, Quantum kicked rotor and its variants: Chaos, localization and beyond, Phys. Rep. 956, 1 (2022).
  47. S. Wimberger, Nonlinear Dynamics and Quantum Chaos (Springer, Berlin, 2014).
  48. V. Karle, A. Ghazaryan, and M. Lemeshko, Topological charges of periodically kicked molecules, Phys. Rev. Lett. 130, 103202 (2023).
  49. C. P. Koch, M. Lemeshko, and D. Sugny, Quantum control of molecular rotation, Rev. Mod. Phys. 91, 035005 (2019).
  50. J. Floß and I. S. Averbukh, Edge states of periodically kicked quantum rotors, Phys. Rev. E 91, 052911 (2015).
  51. M. Bitter and V. Milner, Control of quantum localization and classical diffusion in laser-kicked molecular rotors, Phys. Rev. A 95, 013401 (2017).
  52. Y. Ma, K. E. Khosla, B. A. Stickler, and M. S. Kim, Quantum persistent tennis racket dynamics of nanorotors, Phys. Rev. Lett. 125, 053604 (2020).
  53. These pulses instigate Raman transitions, leading to transitions between different angular momentum states. The pulse power and duration, rather than the energy difference (which increases linearly for angular momenta), are significant, as the pulses are off-resonant. This simplifies the construction of an artificial lattice without the need for multiple pulses with different energies.
  54. In Ref. [57], it has been shown explicitly under which circumstances the sudden-pulse approximation is applicable.
  55. L. Cai and B. Friedrich, Recurring molecular alignment induced by pulsed nonresonant laser fields, Collect. Czech. Chem. Commun. 66, 991 (2001).
  56. C. M. Dion, A. Keller, O. Atabek, and A. D. Bandrauk, Laser-induced alignment dynamics of HCN: Roles of the permanent dipole moment and the polarizability, Phys. Rev. A 59, 1382 (1999).
  57. V. Karle and M. Lemeshko, Modeling laser pulses as δ kicks: Reevaluating the impulsive limit in molecular rotational dynamics, Phys. Rev. A 109, 023101 (2024).
  58. An extension of the one-dimensional lattice in l to a two-dimensional case incorporating m∈{−l,⋯,l} is straightforward. However, this extension shall not be addressed here, as it would introduce additional complexity to the phenomenon of interest discussed in this work and left for exploring in future research.
  59. K. Drese and M. Holthaus, Floquet theory for short laser pulses, Eur. Phys. J. D 5, 119 (1999).
  60. The Floquet operator has a gauge freedom when the kick occurs. In the gauge with the single kick in the center, it is easy to see that the system is time-reversal invariant with T=1. It is straightforward to show that, for any time-reversal operator in this gauge Ũ1,⋯,Ũn, the product Ũ1⋯Ũn−1ŨnŨn−1⋯Ũ1 also has time-reversal symmetry.
  61. More strictly, there are a maximum of N energy bands up to accidental symmetries for odd N, and for even N, there are 2N energy bands. The number of bands originates from the periodicity in the lattice of the free rotation 〈l′|e−iτL̂2/τB|l〉=e−iπl(l+1)/Nδll′ as demonstrated in Ref. [48].
  62. The translational invariance of the angular momentum lattice relies on the convergence of the Clebsch-Gordan coefficients to a constant. Ultimately, we see the existence of the topological edge states does not rely on this convergence, as was demonstrated in Ref. [48]. See Supplemental Material for a more comprehensive derivation of the Fourier transform [66].
  63. K. Wintersperger, C. Braun, F. N. Ünal, A. Eckardt, M. D. Liberto, N. Goldman, I. Bloch, and M. Aidelsburger, Realization of an anomalous Floquet topological system with ultracold atoms, Nat. Phys. 16, 1058 (2020).
  64. P. Titum, E. Berg, M. S. Rudner, G. Refael, and N. H. Lindner, Anomalous Floquet-Anderson insulator as a nonadiabatic quantized charge pump, Phys. Rev. X 6, 021013 (2016).
  65. F. Nathan, D. Abanin, E. Berg, N. H. Lindner, and M. S. Rudner, Anomalous Floquet insulators, Phys. Rev. B 99, 195133 (2019).
  66. See Supplemental Material at https://link.aps.org/supplemental/10.1103/db9d-9bns for detailed derivations.
  67. M. F. Martínez and F. N. Ünal, Wave-packet dynamics and edge transport in anomalous Floquet topological phases, Phys. Rev. A 108, 063314 (2023).
  68. J. Zak, Berry's phase for energy bands in solids, Phys. Rev. Lett. 62, 2747 (1989).
  69. Edge states are localized at two distinct boundaries: l=0 and l=lmax, where lmax is system dependent. Notably, these edge states are not degenerate due to the system's imperfect translational invariance and particularly minor inhomogeneities at the boundaries as detailed in Ref. [66].
  70. Here we define for x,y∈R the 2π-remainder norm |x−y|2π=minn∈Z|x−y+2πn|, which gives the minimal distance on the circle between radiants xandy.
  71. We choose a parametrization α(t) with a smooth function, f(x,y,β)=[1+5β(x+1),0.4+2β(x+1),0.7+3β4(y+1),0.7+3β2(y+1)], noting that this phenomenon is observable for a wide range of parameters and is not a fine-tuned example.
  72. A. Bouhon and R.-J. Slager, Multi-gap topological conversion of Euler class via band-node braiding: Minimal models, PT-linked nodal rings, and chiral heirs, arXiv:2203.16741.
  73. O. A. Alsaiari, A. Bouhon, R.-J. Slager, and F. Nur Ünal, Non-periodic boundary conditions for Euler class and dynamical signatures of obstruction, arXiv:2507.22874.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation