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

Spectroscopy of edge and bulk collective modes in fractional Chern insulators

F. Binanti1, N. Goldman2,3, and C. Repellin4

  • 1University Grenoble-Alpes, CNRS, LPMMC, 38000 Grenoble, France
  • 2CENOLI, Université Libre de Bruxelles, CP 231, Campus Plaine, B-1050 Brussels, Belgium
  • 3Laboratoire Kastler Brossel, Collège de France, CNRS, ENS-Université PSL, Sorbonne Université, 11 Place Marcelin Berthelot, 75005 Paris, France
  • 4Univeristy Grenoble-Alpes, CNRS, LPMMC, 38000 Grenoble, France

Phys. Rev. Research 6, L012054 – Published 8 March, 2024

DOI: https://doi.org/10.1103/PhysRevResearch.6.L012054

Abstract

The exploration of atomic fractional quantum Hall (FQH) states is now within reach in optical-lattice experiments. While ground-state signatures have been observed in a system realizing the Hofstadter-Bose-Hubbard model in a box [Léonard et al., Nature (London) 619, 495 (2023)], how to access hallmark low-energy collective modes remains a central open question in this context. We introduce a spectroscopic scheme based on two interfering Laguerre-Gaussian beams, which transfer a controlled angular momentum and energy to the system. The edge and bulk responses to the probe are detected through local density measurements by tracking the transfer of atoms between the bulk and the edge of the FQH droplet. This detection scheme is shown to simultaneously reveal two specific signatures of FQH states: their chiral edge branch and their bulk magnetoroton mode. We numerically benchmark our method by considering few bosons in the ν=1/2 Laughlin ground state of the Hofstadter-Bose-Hubbard model, and demonstrate that these signatures are already detectable in realistic systems of two bosons, provided that the box potential is sufficiently large compared to the droplet. Our paper paves the way for the detection of fractional statistics in cold atoms through edge signatures.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (63)

  1. J. Dalibard, F. Gerbier, G. Juzeliūnas, and P. Öhberg, Colloquium: Artificial gauge potentials for neutral atoms, Rev. Mod. Phys. 83, 1523 (2011).
  2. N. Goldman, G. Juzeliūnas, P. Öhberg, and I. B. Spielman, Light-induced gauge fields for ultracold atoms, Rep. Prog. Phys. 77, 126401 (2014).
  3. N. R. Cooper, J. Dalibard, and I. B. Spielman, Topological bands for ultracold atoms, Rev. Mod. Phys. 91, 015005 (2019).
  4. M. Popp, B. Paredes, and J. I. Cirac, Adiabatic path to fractional quantum Hall states of a few bosonic atoms, Phys. Rev. A 70, 053612 (2004).
  5. N. R. Cooper and J. Dalibard, Reaching fractional quantum Hall states with optical flux lattices, Phys. Rev. Lett. 110, 185301 (2013).
  6. N. Y. Yao, A. V. Gorshkov, C. R. Laumann, A. M. Läuchli, J. Ye, and M. D. Lukin, Realizing fractional Chern insulators in dipolar spin systems, Phys. Rev. Lett. 110, 185302 (2013).
  7. F. Grusdt, F. Letscher, M. Hafezi, and M. Fleischhauer, Topological growing of Laughlin states in synthetic gauge fields, Phys. Rev. Lett. 113, 155301 (2014).
  8. Y.-C. He, F. Grusdt, A. Kaufman, M. Greiner, and A. Vishwanath, Realizing and adiabatically preparing bosonic integer and fractional quantum Hall states in optical lattices, Phys. Rev. B 96, 201103(R) (2017).
  9. C. Repellin, T. Yefsah, and A. Sterdyniak, Creating a bosonic fractional quantum Hall state by pairing fermions, Phys. Rev. B 96, 161111(R) (2017).
  10. J. Motruk and F. Pollmann, Phase transitions and adiabatic preparation of a fractionalChern insulator in a boson cold-atom model, Phys. Rev. B 96, 165107 (2017).
  11. A. Hudomal, N. Regnault, and I. Vasić, Bosonic fractional quantum Hall states in driven optical lattices, Phys. Rev. A 100, 053624 (2019).
  12. B. Michen, C. Repellin, and J. C. Budich, Adiabatic preparation of fractional Chern insulators from an effective thin-torus limit, Phys. Rev. Res. 5, 023100 (2023).
  13. C. Repellin and N. Goldman, Detecting fractional Chern insulators through circular dichroism, Phys. Rev. Lett. 122, 166801 (2019).
  14. C. Repellin, J. Léonard, and N. Goldman, Fractional Chern insulators of few bosons in a box: Hall plateaus from center-of-mass drifts and density profiles, Phys. Rev. A 102, 063316 (2020).
  15. J. Motruk and I. Na, Detecting fractional Chern insulators in optical lattices through quantized displacement, Phys. Rev. Lett. 125, 236401 (2020).
  16. Z.-P. Cian, H. Dehghani, A. Elben, B. Vermersch, G. Zhu, M. Barkeshli, P. Zoller, and M. Hafezi, Many-body Chern number from statistical correlations of randomized measurements, Phys. Rev. Lett. 126, 050501 (2021).
  17. F. A. Palm, S. Mardazad, A. Bohrdt, U. Schollwöck, and F. Grusdt, Snapshot-based detection of ν=12 Laughlin states: Coupled chains and central charge, Phys. Rev. B 106, L081108 (2022).
  18. N. R. Cooper and S. H. Simon, Signatures of fractional exclusion statistics in the spectroscopy of quantum Hall droplets, Phys. Rev. Lett. 114, 106802 (2015).
  19. M. Račiūnas, F. N. Ünal, E. Anisimovas, and A. Eckardt, Creating, probing, and manipulating fractionally charged excitations of fractional Chern insulators in optical lattices, Phys. Rev. A 98, 063621 (2018).
  20. R. O. Umucalılar, E. Macaluso, T. Comparin, and I. Carusotto, Time-of-flight measurements as a possible method to observe anyonic statistics, Phys. Rev. Lett. 120, 230403 (2018).
  21. E. Macaluso, T. Comparin, R. O. Umucalılar, M. Gerster, S. Montangero, M. Rizzi, and I. Carusotto, Charge and statistics of lattice quasiholes from density measurements: A tree tensor network study, Phys. Rev. Res. 2, 013145 (2020).
  22. B. Wang, X.-Y. Dong, and A. Eckardt, Measurable signatures of bosonic fractional Chern insulator states and their fractional excitations in a quantum-gas microscope, SciPost Phys. 12, 095 (2022).
  23. X. Li, B. Jaworowski, M. Haque, and A. E. B. Nielsen, Dynamics of quasiholes and quasiparticles at the edges of small lattices, Phys. Rev. A 109, 023312 (2024).
  24. J. Léonard, S. Kim, J. Kwan, P. Segura, F. Grusdt, C. Repellin, N. Goldman, and M. Greiner, Realization of a fractional quantum Hall state with ultracold atoms, Nature (London) 619, 495 (2023).
  25. X. G. Wen, Chiral Luttinger liquid and the edge excitations in the fractional quantum Hall states, Phys. Rev. B 41, 12838 (1990).
  26. C. Bäuerle, D. C. Glattli, T. Meunier, F. Portier, P. Roche, P. Roulleau, S. Takada, and X. Waintal, Coherent control of single electrons: A review of current progress, Rep. Prog. Phys. 81, 056503 (2018).
  27. E. Macaluso and I. Carusotto, Hard-wall confinement of a fractional quantum Hall liquid, Phys. Rev. A 96, 043607 (2017).
  28. R. Fern and S. H. Simon, Quantum Hall edges with hard confinement: Exact solution beyond Luttinger liquid, Phys. Rev. B 95, 201108(R) (2017).
  29. X.-Y. Dong, A. G. Grushin, J. Motruk, and F. Pollmann, Charge excitation dynamics in bosonic fractional Chern insulators, Phys. Rev. Lett. 121, 086401 (2018).
  30. A. Nardin and I. Carusotto, Linear and nonlinear edge dynamics of trapped fractional quantum Hall droplets, Phys. Rev. A 107, 033320 (2023).
  31. B. Oblak, B. Lapierre, P. Moosavi, J.-M. Stéphan, and B. Estienne, Anisotropic quantum Hall droplets, arXiv:2301.01726.
  32. J. A. Kjäll and J. E. Moore, Edge excitations of bosonic fractional quantum Hall phases in optical lattices, Phys. Rev. B 85, 235137 (2012).
  33. W.-W. Luo, W.-C. Chen, Y.-F. Wang, and C.-D. Gong, Edge excitations in fractional Chern insulators, Phys. Rev. B 88, 161109(R) (2013).
  34. S. M. Girvin, A. H. MacDonald, and P. M. Platzman, Collective-excitation gap in the fractional quantum Hall effect, Phys. Rev. Lett. 54, 581 (1985).
  35. S. M. Girvin, A. H. MacDonald, and P. M. Platzman, Magneto-roton theory of collective excitations in the fractional quantum Hall effect, Phys. Rev. B 33, 2481 (1986).
  36. G. Moore and N. Read, Nonabelions in the fractional quantumHall effect, Nucl. Phys. B 360, 362 (1991).
  37. X.-G. Wen, Topological order and edge structure of ν=1/2 quantum Hall state, Phys. Rev. Lett. 70, 355 (1993).
  38. M. Milovanović and N. Read, Edge excitations of paired fractional quantum Hall states, Phys. Rev. B 53, 13559 (1996).
  39. R. K. Kamilla, X. G. Wu, and J. K. Jain, Excitons of composite fermions, Phys. Rev. B 54, 4873 (1996).
  40. I. D. Rodriguez, A. Sterdyniak, M. Hermanns, J. K. Slingerland, and N. Regnault, Quasiparticles and excitons for the Pfaffian quantum Hall state, Phys. Rev. B 85, 035128 (2012).
  41. B. Yang, Z.-X. Hu, Z. Papić, and F. D. M. Haldane, Model wave functions for the collective modes and the magnetoroton theory of the fractional quantum Hall effect, Phys. Rev. Lett. 108, 256807 (2012).
  42. B. Yang, Analytic wave functions for neutral bulk excitations in fractional quantum Hall fluids, Phys. Rev. B 87, 245132 (2013).
  43. T. Jolicoeur, Shape of the magnetoroton at ν=1/3 and ν=7/3 in real samples, Phys. Rev. B 95, 075201 (2017).
  44. M. Mancini, G. Pagano, G. Cappellini, L. Livi, M. Rider, J. Catani, C. Sias, P. Zoller, M. Inguscio, M. Dalmonte, and L. Fallani, Observation of chiral edge states with neutral fermions in synthetic Hall ribbons, Science 349, 1510 (2015).
  45. B. K. Stuhl, H.-I. Lu, L. M. Aycock, D. Genkina, and I. B. Spielman, Visualizing edge states with an atomic Bose gas in the quantum Hall regime, Science 349, 1514 (2015).
  46. T. Chalopin, T. Satoor, A. Evrard, V. Makhalov, J. Dalibard, R. Lopes, and S. Nascimbene, Probing chiral edge dynamics and bulk topology of a synthetic Hall system, Nat. Phys. 16, 1017 (2020).
  47. C. Braun, R. Saint-Jalm, A. Hesse, J. Arceri, I. Bloch, and M. Aidelsburger, Real-space detection and manipulation of topological edge modes with ultracold atoms, arXiv:2304.01980.
  48. R. Yao, S. Chi, B. Mukherjee, A. Shaffer, M. Zwierlein, and R. J. Fletcher, Observation of chiral edge transport in a rapidly-rotating quantum gas, arXiv:2304.10468.
  49. N. Goldman, J. Beugnon, and F. Gerbier, Detecting chiral edge states in the Hofstadter optical lattice, Phys. Rev. Lett. 108, 255303 (2012).
  50. M. E. Tai, A. Lukin, M. Rispoli, R. Schittko, T. Menke, Dan Borgnia, P. M. Preiss, F. Grusdt, A. M. Kaufman, and M. Greiner, Microscopy of the interacting Harper-Hofstadter model in the two-body limit, Nature (London) 546, 519 (2017).
  51. A. S. Sorensen, E. Demler, and M. D. Lukin, Fractional quantum Hall states of atoms in optical lattices, Phys. Rev. Lett. 94, 086803 (2005).
  52. M. Hafezi, A. S. Sørensen, E. Demler, and M. D. Lukin, Fractional quantum Hall effect in optical lattices, Phys. Rev. A 76, 023613 (2007).
  53. M. Gerster, M. Rizzi, P. Silvi, M. Dalmonte, and S. Montangero, Fractional quantum Hall effect in the interacting Hofstadter model via tensor networks, Phys. Rev. B 96, 195123 (2017).
  54. D. R. Hofstadter, Energy levels and wave functions of Bloch electrons in rational and irrational magnetic fields, Phys. Rev. B 14, 2239 (1976).
  55. A. Nardin, R. Lopes, M. Rizzi, L. Mazza, and S. Nascimbene, Bisognano-Wichmann Hamiltonian for the entanglement spectroscopy of fractional quantum Hall states, arXiv:2312.07604.
  56. For two particles, the counting for a free chiral boson (1, 1, 2, 3, 5, 7 ...) is truncated down to (1, 1, 2, 2, 3, 3 ...).
  57. T. Ozawa, H. M. Price, and I. Carusotto, Momentum-space Harper-Hofstadter model, Phys. Rev. A 92, 023609 (2015).
  58. H. He, M. E. J. Friese, N. R. Heckenberg, and H. Rubinsztein-Dunlop, Direct observation of transfer of angular momentum to absorptive particles from a laser beam with a phase singularity, Phys. Rev. Lett. 75, 826 (1995).
  59. B.-Y. Sun, N. Goldman, M. Aidelsburger, and M. Bukov, Engineering and probing non-Abelian chiral spin liquids using periodically driven ultracold atoms, PRX Quantum 4, 020329 (2023).
  60. C. Repellin, T. Neupert, Z. Papić, and N. Regnault, Single-mode approximation for fractional Chern insulators and the fractional quantum Hall effect on the torus, Phys. Rev. B 90, 045114 (2014).
  61. See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevResearch.6.L012054 for additional numerical results, including the influence of lattice effects, time-dependent simulations in the configuration of the Harvard experiment, local density patterns, and absorption spectra for three and four bosons.
  62. The counting is, respectively, (1, 1, 2, 3) and (1, 1, 3, 5) for the Laughlin and Moore-Read states.
  63. Lmax=N and Lmax=N/2 are, respectively, expected for Laughlin and Moore-Read.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation