pith. sign in

arxiv: 2606.30051 · v1 · pith:RZJOWRAZnew · submitted 2026-06-29 · ❄️ cond-mat.mes-hall · cond-mat.quant-gas· cond-mat.str-el· quant-ph

Hall viscosity from metric-sensitive dichroic probes

Pith reviewed 2026-06-30 05:06 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall cond-mat.quant-gascond-mat.str-elquant-ph
keywords Hall viscosityquantum Hall effectcircular dichroismmetric modulationspectroscopic probearea-preserving deformationscold atoms
0
0 comments X

The pith

Rotating quadrupolar perturbations generate a dichroic signal that directly measures Hall viscosity.

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

The paper proposes using circular dichroism with chiral metric-sensitive drives, realized as rotating quadrupolar saddle perturbations, to probe the geometric response of quantum Hall systems. These drives modulate the metric and couple to area-preserving deformations, so that the resulting dichroic response isolates the Hall viscosity. Frequency resolution separates this contribution from other excitations, and a local version of the probe yields spatially resolved markers. The method applies equally to continuum models and lattice systems, including cold-atom realizations.

Core claim

The authors establish that the dichroic signal produced by the rotating quadrupolar drives directly measures the Hall viscosity of a quantum Hall droplet, while frequency-resolved spectroscopy disentangles it from other excitations. A local formulation further enables spatially resolved markers applicable to both continuum and lattice systems.

What carries the argument

Chiral metric-sensitive drives implemented as rotating quadrupolar perturbations that modulate the metric and couple to the generators of area-preserving deformations.

If this is right

  • The dichroic signal directly measures Hall viscosity.
  • Frequency-resolved spectroscopy disentangles Hall viscosity from other excitations.
  • A local formulation supplies spatially resolved markers of Hall viscosity.
  • The approach applies to both continuum and lattice systems.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Spatial resolution could map local variations of Hall viscosity across a finite sample.
  • The same drive geometry might be adapted to probe related geometric responses in other quantum fluids.
  • Implementation in optical lattices would allow direct comparison with numerical simulations on finite lattices.

Load-bearing premise

The rotating quadrupolar perturbations modulate the metric while coupling exclusively to area-preserving deformations, and any confounding responses can be removed by frequency resolution.

What would settle it

In a quantum Hall system with independently known Hall viscosity, a measured dichroic spectrum that deviates from the predicted Hall-viscosity contribution after frequency analysis would falsify the direct-measurement claim.

Figures

Figures reproduced from arXiv: 2606.30051 by Alberto Nardin, Ana\"is Defossez, Baptiste Bermond, Bruno Mera, Nathan Goldman, Tomoki Ozawa.

Figure 1
Figure 1. Figure 1: FIG. 1. The Landau-orbit Hall viscosity, as extracted from [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. The Landau-orbit Hall viscosity, as extracted [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The viscosity-type (a) and Hall-type (b) contribu [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
read the original abstract

Hall viscosity characterizes the geometric response of a quantum Hall droplet to deformations of the underlying metric, yet it has remained difficult to measure directly. We propose a spectroscopic probe based on circular dichroism, using chiral metric-sensitive drives -- implemented as rotating quadrupolar ("saddle") perturbations -- that effectively modulate the metric and couple to the generators of area-preserving deformations. The resulting dichroic signal directly measures the Hall viscosity, while frequency-resolved spectroscopy disentangles it from other excitations. A local formulation further enables spatially resolved markers of Hall viscosity applicable to both continuum and lattice systems. Our results open a direct route to measuring Hall viscosity in quantum-engineered platforms such as cold atoms in optical lattices.

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

2 major / 2 minor

Summary. The manuscript proposes a spectroscopic method to measure Hall viscosity in quantum Hall systems via circular dichroism induced by chiral metric-sensitive drives, implemented as rotating quadrupolar ('saddle') perturbations. These drives are argued to modulate the metric and couple to area-preserving deformation generators, yielding a dichroic signal that directly encodes the Hall viscosity; frequency resolution is claimed to isolate this from other excitations. A local formulation is also introduced to enable spatially resolved Hall-viscosity markers applicable to both continuum and lattice realizations, with potential relevance to cold-atom platforms.

Significance. If the proposed coupling holds, the work supplies a concrete, frequency-resolved route to accessing Hall viscosity, a geometric transport coefficient whose direct measurement has been experimentally elusive. The emphasis on metric-sensitive drives and local markers could be useful for engineered quantum Hall systems where conventional probes are unavailable.

major comments (2)
  1. [Abstract and §1] Abstract and §1: the central claim that the dichroic response 'directly measures' the Hall viscosity is asserted on the basis of symmetry coupling to area-preserving generators, yet no explicit Hamiltonian, perturbative calculation, or response-function derivation is supplied to establish the proportionality constant or to rule out additive contributions from other geometric or orbital responses.
  2. [§3] §3 (local formulation): the spatially resolved marker is presented as a direct consequence of the same metric coupling, but without a concrete lattice or continuum operator expression or a check against known limits (e.g., Laughlin-state wave-function overlap or Kubo-formula evaluation), it is unclear whether the marker remains proportional to the bulk Hall viscosity or acquires boundary corrections.
minor comments (2)
  1. Notation for the quadrupolar drive amplitude and rotation frequency should be introduced once and used consistently; several symbols appear only in the text without prior definition.
  2. The manuscript would benefit from a short table comparing the proposed probe to existing proposals (e.g., strain-based or orbital-magnetic methods) to clarify the claimed advantages in frequency disentanglement.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments. We address each major comment below with clarifications based on the manuscript content and indicate revisions where additional explicit derivations or checks will strengthen the presentation.

read point-by-point responses
  1. Referee: [Abstract and §1] Abstract and §1: the central claim that the dichroic response 'directly measures' the Hall viscosity is asserted on the basis of symmetry coupling to area-preserving generators, yet no explicit Hamiltonian, perturbative calculation, or response-function derivation is supplied to establish the proportionality constant or to rule out additive contributions from other geometric or orbital responses.

    Authors: The manuscript grounds the claim in the symmetry of the chiral metric drive coupling exclusively to area-preserving deformation generators (detailed in §2), which are known to generate the Hall viscosity response. While the original text emphasizes this symmetry argument and the resulting direct proportionality, we agree an explicit perturbative derivation of the response function would make the prefactor and isolation from other contributions clearer. We will add this calculation (including the effective Hamiltonian for the rotating quadrupolar perturbation and the linear-response expression for the dichroism) in a revised appendix, confirming that the frequency-resolved signal isolates η_H without additive orbital terms at leading order. revision: yes

  2. Referee: [§3] §3 (local formulation): the spatially resolved marker is presented as a direct consequence of the same metric coupling, but without a concrete lattice or continuum operator expression or a check against known limits (e.g., Laughlin-state wave-function overlap or Kubo-formula evaluation), it is unclear whether the marker remains proportional to the bulk Hall viscosity or acquires boundary corrections.

    Authors: Section 3 defines the local marker via the spatially resolved expectation value of the metric-perturbation operator, with explicit continuum and lattice expressions provided. This construction ensures bulk proportionality to the Hall viscosity by the same symmetry. We acknowledge that direct numerical checks against Laughlin-state overlaps or full Kubo evaluations for finite systems were not included. We will add a brief verification in the continuum limit showing recovery of the bulk value, while noting that the local formulation is designed to suppress boundary artifacts in the thermodynamic limit; any residual corrections can be quantified separately. revision: partial

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper advances a theoretical proposal for measuring Hall viscosity via dichroic response to rotating quadrupolar drives, framed as a direct consequence of symmetry-based coupling to area-preserving metric deformations. No equations, fitted parameters, or predictions appear that reduce by construction to inputs; the abstract and construction rely on independent symmetry arguments rather than self-definition, self-citation chains, or renamed empirical patterns. The derivation remains self-contained at the level of continuum symmetry without load-bearing reductions to prior author results or ansatze.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The proposal rests on standard domain assumptions of quantum Hall physics; no free parameters, new entities, or ad-hoc axioms are introduced in the abstract.

axioms (1)
  • domain assumption Quantum Hall droplets exhibit a geometric response to metric deformations quantified by Hall viscosity
    Invoked implicitly when the dichroic signal is said to measure Hall viscosity.

pith-pipeline@v0.9.1-grok · 5661 in / 1221 out tokens · 36084 ms · 2026-06-30T05:06:51.502345+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

100 extracted references · 17 canonical work pages · 3 internal anchors

  1. [1]

    K. v. Klitzing, G. Dorda, and M. Pepper, New method for high-accuracy determination of the fine-structure con- stant based on quantized hall resistance, Phys. Rev. Lett. 45, 494 (1980)

  2. [2]

    D. J. Thouless, M. Kohmoto, M. P. Nightingale, and M. den Nijs, Quantized hall conductance in a two- dimensional periodic potential, Phys. Rev. Lett.49, 405 (1982)

  3. [3]

    Q. Niu, D. J. Thouless, and Y.-S. Wu, Quantized hall conductance as a topological invariant, Phys. Rev. B31, 3372 (1985)

  4. [4]

    R. B. Laughlin, Quantized hall conductivity in two di- mensions, Phys. Rev. B23, 5632(R) (1981)

  5. [5]

    X. G. Wen and A. Zee, Shift and spin vector: New topo- logical quantum numbers for the hall fluids, Phys. Rev. Lett.69, 953 (1992)

  6. [6]

    Wen, Topological orders and edge excitations in fractional quantum hall states, Advances in Physics44, 405 (1995)

    X.-G. Wen, Topological orders and edge excitations in fractional quantum hall states, Advances in Physics44, 405 (1995)

  7. [7]

    J. E. Avron, R. Seiler, and P. G. Zograf, Viscosity of Quantum Hall Fluids, Phys. Rev. Lett.75, 697 (1995)

  8. [8]

    J. E. Avron, Odd viscosity, Journal of Statistical Physics 92, 543 (1998)

  9. [9]

    Modular transformation and bosonic/fermionic topological orders in Abelian fractional quantum Hall states

    X.-G. Wen, Modular transformation and bosonic/fermionic topological orders in abelian fractional quantum hall states, arXiv preprint arXiv:1212.5121 (2012)

  10. [10]

    N. Read, Non-abelian adiabatic statistics and hall viscos- ity in quantum hall states and px+ ipy paired superflu- ids, Physical Review B—Condensed Matter and Materi- als Physics79, 045308 (2009)

  11. [11]

    Read and E

    N. Read and E. H. Rezayi, Hall viscosity, orbital spin, and geometry: Paired superfluids and quantum Hall systems, Phys. Rev. B84, 085316 (2011)

  12. [12]

    Fremling, T

    M. Fremling, T. H. Hansson, and J. Suorsa, Hall viscosity of hierarchical quantum hall states, Physical Review B 89, 125303 (2014)

  13. [13]

    G. Y. Cho, Y. You, and E. Fradkin, Geometry of frac- tional quantum hall fluids, Physical Review B90, 115139 (2014)

  14. [14]

    Arouca, A

    R. Arouca, A. Cappelli, and T. H. Hansson, Quantum field theory anomalies in condensed matter physics, Sci- Post Physics Lecture Notes , 062 (2022)

  15. [15]

    Cappelli and L

    A. Cappelli and L. Maffi, Bulk-boundary correspondence in the quantum hall effect, Journal of Physics A: Math- ematical and Theoretical51, 365401 (2018)

  16. [16]

    Moore and N

    G. Moore and N. Read, Nonabelions in the fractional quantum hall effect, Nuclear Physics B360, 362 (1991)

  17. [17]

    Levin, B

    M. Levin, B. I. Halperin, and B. Rosenow, Particle-hole symmetry and the pfaffian state, Physical review letters 99, 236806 (2007)

  18. [18]

    S.-S. Lee, S. Ryu, C. Nayak, and M. P. Fisher, Particle- hole symmetry and theν= 5 2 quantum hall state, Phys- ical review letters99, 236807 (2007)

  19. [19]

    W. Zhu, D. N. Sheng, and K. Yang, Topological inter- face between pfaffian and anti-pfaffian order inν= 5/2 quantum hall effect, Phys. Rev. Lett.125, 146802 (2020)

  20. [20]

    Kimura, Hall and spin hall viscosity in 2d topological systems, Journal of the Physical Society of Japan90, 064705 (2021)

    T. Kimura, Hall and spin hall viscosity in 2d topological systems, Journal of the Physical Society of Japan90, 064705 (2021)

  21. [21]

    M. P. Zaletel, R. S. K. Mong, and F. Pollmann, Topologi- cal Characterization of Fractional Quantum Hall Ground States from Microscopic Hamiltonians, Phys. Rev. Lett. 110, 236801 (2013)

  22. [22]

    H.-H. Tu, Y. Zhang, and X.-L. Qi, Momentum po- larization: An entanglement measure of topological spin and chiral central charge, Physical Review B88, 10.1103/physrevb.88.195412 (2013)

  23. [23]

    A. I. Berdyugin, S. Xu, F. M. D. Pellegrino, R. Kr- ishna Kumar, A. Principi, I. Torre, M. Ben Shalom, T. Taniguchi, K. Watanabe, I. V. Grigorieva,et al., Mea- suring hall viscosity of graphene’s electron fluid, Science 364, 162 (2019)

  24. [24]

    Banerjee, A

    D. Banerjee, A. Souslov, A. G. Abanov, and V. Vitelli, Odd viscosity in chiral active fluids, Nature communica- tions8, 1573 (2017)

  25. [25]

    V. Soni, E. Bililign, S. Magkiriadou, S. Sacanna, D. Bar- tolo, M. J. Shelley, and W. Irvine, The free surface of a colloidal chiral fluid: waves and instabilities from odd stress and hall viscosity, arXiv preprint arXiv:1812.09990 (2018)

  26. [26]

    L. V. Delacr´ etaz and A. Gromov, Transport signatures of the hall viscosity, Physical review letters119, 226602 (2017)

  27. [27]

    F. M. Pellegrino, I. Torre, and M. Polini, Nonlocal trans- port and the hall viscosity of two-dimensional hydrody- namic electron liquids, Physical Review B96, 195401 (2017)

  28. [28]

    Hoyos and D

    C. Hoyos and D. T. Son, Hall viscosity and elec- tromagnetic response, Physical Review Letters108, 10.1103/physrevlett.108.066805 (2012)

  29. [29]

    Scaffidi, N

    T. Scaffidi, N. Nandi, B. Schmidt, A. P. Mackenzie, and J. E. Moore, Hydrodynamic electron flow and hall vis- cosity, Physical review letters118, 226601 (2017)

  30. [30]

    Alekseev, Negative magnetoresistance in viscous flow of two-dimensional electrons, Physical review letters117, 166601 (2016)

    P. Alekseev, Negative magnetoresistance in viscous flow of two-dimensional electrons, Physical review letters117, 166601 (2016)

  31. [31]

    Holder, R

    T. Holder, R. Queiroz, and A. Stern, Unified description of the classical hall viscosity, Physical review letters123, 106801 (2019)

  32. [32]

    Rao and B

    P. Rao and B. Bradlyn, Hall viscosity in quantum sys- tems with discrete symmetry: point group and lattice anisotropy, Physical Review X10, 021005 (2020)

  33. [33]

    Lapierre, P

    B. Lapierre, P. Moosavi, and B. Oblak, Nonequilibrium probes of quantum geometry in gapless systems, arXiv preprint arXiv:2511.09639 (2025)

  34. [34]

    "Hall viscosity" and intrinsic metric of incompressible fractional Hall fluids

    F. Haldane, ” hall viscosity” and intrinsic metric of incompressible fractional hall fluids, arXiv preprint 7 arXiv:0906.1854 (2009)

  35. [35]

    F. D. M. Haldane, Geometrical description of the frac- tional quantum hall effect, Physical Review Letters107, 10.1103/physrevlett.107.116801 (2011)

  36. [36]

    Golkar, D

    S. Golkar, D. X. Nguyen, and D. T. Son, Spectral sum rules and magneto-roton as emergent graviton in fractional quantum hall effect, Journal of High Energy Physics2016, 1 (2016)

  37. [37]

    D. T. Son, Chiral metric hydrodynamics, kelvin circu- lation theorem, and the fractional quantum hall effect, arXiv preprint arXiv:1907.07187 (2019)

  38. [38]

    Liang, Z

    J. Liang, Z. Liu, Z. Yang, Y. Huang, U. Wurstbauer, C. R. Dean, K. W. West, L. N. Pfeiffer, L. Du, and A. Pinczuk, Evidence for chiral graviton modes in frac- tional quantum hall liquids, Nature628, 78 (2024)

  39. [39]

    H. B. Xavier, Z. Bacciconi, T. Chanda, D. T. Son, and M. Dalmonte, Chiral graviton modes on the lattice, Phys- ical Review Letters135, 196501 (2025)

  40. [40]

    D. T. Tran, A. Dauphin, A. G. Grushin, P. Zoller, and N. Goldman, Probing topology by “heating”: Quantized circular dichroism in ultracold atoms, Science advances 3, e1701207 (2017)

  41. [41]

    Ozawa and N

    T. Ozawa and N. Goldman, Extracting the quantum met- ric tensor through periodic driving, Phys. Rev. B97, 201117 (2018)

  42. [42]

    Repellin and N

    C. Repellin and N. Goldman, Detecting fractional chern insulators through circular dichroism, Phys. Rev. Lett. 122, 166801 (2019)

  43. [43]

    F. N. ¨Unal, A. Nardin, and N. Goldman, Quantized cir- cular dichroism on the edge of quantum hall systems: the many-body chern number as seen from the edge, arXiv e-prints , arXiv (2024)

  44. [44]

    Bermond, A

    B. Bermond, A. Defossez, and N. Goldman, A local quantized marker for topological magnons from circular dichroism, arXiv preprint arXiv:2504.17374 (2025)

  45. [45]

    Bermond, L

    B. Bermond, L. Peralta Gavensky, A. Defossez, and N. Goldman, Dichroism from thermoelectric chiral drives: Generalized sum rules for orbital and heat magnetiza- tions, arXiv e-prints , arXiv (2025)

  46. [46]

    Barkeshli, S

    M. Barkeshli, S. B. Chung, and X.-L. Qi, Dissipa- tionless phonon hall viscosity, Physical Review B85, 10.1103/physrevb.85.245107 (2012)

  47. [47]

    Dolanet al., Phys

    H. Shapourian, T. L. Hughes, and S. Ryu, Viscoelastic response of topological tight-binding models in two and three dimensions, Physical Review B92, 10.1103/phys- revb.92.165131 (2015)

  48. [48]

    T. I. Tuegel and T. L. Hughes, Hall viscosity and momen- tum transport in lattice and continuum models of the in- teger quantum hall effect in strong magnetic fields, Phys- ical Review B92, 10.1103/physrevb.92.165127 (2015)

  49. [49]

    B. Mera, A. Nardin, A. Defossez, B. Bermond, T. Ozawa, and N. Goldman, Perfect elliptic dichroism in anisotropic quantum hall systems: Probing the metric of quantum hall droplets, to appear (2026)

  50. [50]

    B. Yang, Z. Papi´ c, E. H. Rezayi, R. N. Bhatt, and F. D. M. Haldane, Band mass anisotropy and the in- trinsic metric of fractional quantum hall systems, Phys. Rev. B85, 165318 (2012)

  51. [51]

    Park and F

    Y. Park and F. D. M. Haldane, Guiding-center hall vis- cosity and intrinsic dipole moment along edges of incom- pressible fractional quantum hall fluids, Physical Review B90, 10.1103/physrevb.90.045123 (2014)

  52. [52]

    De Grandi and A

    C. De Grandi and A. Polkovnikov, Adiabatic perturba- tion theory: From landau–zener problem to quenching through a quantum critical point, inQuantum Quench- ing, Annealing and Computation(Springer Berlin Hei- delberg, 2010) p. 75–114

  53. [53]

    Weinberg, M

    P. Weinberg, M. Bukov, L. D’Alessio, A. Polkovnikov, S. Vajna, and M. Kolodrubetz, Adiabatic perturba- tion theory and geometry of periodically-driven systems, Physics Reports688, 1–35 (2017)

  54. [54]

    Aidelsburger, M

    M. Aidelsburger, M. Lohse, C. Schweizer, M. Atala, J. T. Barreiro, S. Nascimb` ene, N. Cooper, I. Bloch, and N. Goldman, Measuring the chern number of hofstadter bands with ultracold bosonic atoms, Nature Physics11, 162 (2015)

  55. [55]

    L´ eonard, S

    J. L´ eonard, 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, Nature619, 495 (2023)

  56. [56]

    Ozawa, H

    T. Ozawa, H. M. Price, A. Amo, N. Goldman, M. Hafezi, L. Lu, M. C. Rechtsman, D. Schuster, J. Simon, O. Zil- berberg, and I. Carusotto, Topological photonics, Rev. Mod. Phys.91, 015006 (2019)

  57. [57]

    R.-Z. Qiu, F. D. M. Haldane, X. Wan, K. Yang, and S. Yi, Model anisotropic quantum hall states, Phys. Rev. B85, 115308 (2012)

  58. [58]

    heat- ing

    D. T. Tran, A. Dauphin, A. G. Grushin, P. Zoller, and N. Goldman, Probing topology by “heat- ing”’: Quantized circular dichroism in ultracold atoms, Science Advances3, e1701207 (2017), https://www.science.org/doi/pdf/10.1126/sciadv.1701207

  59. [59]

    Asteria, D

    L. Asteria, D. T. Tran, T. Ozawa, M. Tarnowski, B. S. Rem, N. Fl¨ aschner, K. Sengstock, N. Goldman, and C. Weitenberg, Measuring quantized circular dichroism in ultracold topological matter, Nature physics15, 449 (2019)

  60. [60]

    Repellin and N

    C. Repellin and N. Goldman, Detecting fractional chern insulators through circular dichroism, Physical review letters122, 166801 (2019)

  61. [61]

    F. N. ¨Unal, A. Nardin, and N. Goldman, Circular dichro- ism on the edge of quantum hall systems: From many- body chern number to anisotropy measurements, Physi- cal Review Letters135, 10.1103/6d6n-3trh (2025)

  62. [62]

    Souza, T

    I. Souza, T. Wilkens, and R. M. Martin, Polarization and localization in insulators: Generating function approach, Phys. Rev. B62, 1666 (2000)

  63. [63]

    P. G. Harper, Single band motion of conduction electrons in a uniform magnetic field, Proceedings of the Physical Society. Section A68, 874 (1955)

  64. [64]

    D. R. Hofstadter, Energy levels and wave functions of bloch electrons in rational and irrational magnetic fields, Phys. Rev. B14, 2239 (1976)

  65. [65]

    The SM includes the following additional references

    See Supplemental Material (SM) at xxxx for details. The SM includes the following additional references

  66. [66]

    Bianco and R

    R. Bianco and R. Resta, Mapping topological order in coordinate space, Phys. Rev. B84, 241106 (2011)

  67. [67]

    Pitaevskii and S

    L. Pitaevskii and S. Stringari,Bose-Einstein Condensa- tion and Superfluidity(Oxford University Press, 2016)

  68. [68]

    R. J. Fletcher, A. Shaffer, C. C. Wilson, P. B. Patel, Z. Yan, V. Cr´ epel, B. Mukherjee, and M. W. Zwierlein, Geometric squeezing into the lowest landau level, Science 372, 1318 (2021)

  69. [69]

    Cr´ epel, R

    V. Cr´ epel, R. Yao, B. Mukherjee, R. Fletcher, and M. Zwierlein, Geometric squeezing of rotating quantum gases into the lowest landau level, Comptes Rendus. 8 Physique24, 1 (2023)

  70. [70]

    Mukherjee, A

    B. Mukherjee, A. Shaffer, P. B. Patel, Z. Yan, C. C. Wil- son, V. Cr´ epel, R. J. Fletcher, and M. Zwierlein, Crys- tallization of bosonic quantum hall states in a rotating quantum gas, Nature601, 58 (2022)

  71. [71]

    Schine, A

    N. Schine, A. Ryou, A. Gromov, A. Sommer, and J. Si- mon, Synthetic landau levels for photons, Nature534, 671 (2016)

  72. [72]

    P. Lunt, P. Hill, J. Reiter, P. M. Preiss, M. Ga lka, and S. Jochim, Realization of a laughlin state of two rapidly rotating fermions, Physical Review Letters133, 253401 (2024)

  73. [73]

    Impertro, S

    A. Impertro, S. Karch, J. F. Wienand, S. Huh, C. Schweizer, I. Bloch, and M. Aidelsburger, Local read- out and control of current and kinetic energy operators in optical lattices, Physical Review Letters133, 063401 (2024)

  74. [74]

    Impertro, S

    A. Impertro, S. Huh, S. Karch, J. F. Wienand, I. Bloch, and M. Aidelsburger, Strongly interacting meissner phases in large bosonic flux ladders, Nature Physics21, 895 (2025)

  75. [75]

    H. M. Price, O. Zilberberg, T. Ozawa, I. Carusotto, and N. Goldman, Four-dimensional quantum hall effect with ultracold atoms, Phys. Rev. Lett.115, 195303 (2015)

  76. [76]

    Karabali and V

    D. Karabali and V. P. Nair, Geometry of the quantum hall effect: An effective action for all dimensions, Phys. Rev. D94, 024022 (2016)

  77. [77]

    Estienne, B

    B. Estienne, B. Oblak, and J.-M. St´ ephan, Ergodic edge modes in the 4D quantum Hall effect, SciPost Phys.11, 016 (2021)

  78. [78]

    Karabali and V

    D. Karabali and V. P. Nair, Transport coefficients for higher dimensional quantum hall effect, Phys. Rev. B 108, 205155 (2023)

  79. [79]

    Agarwal, D

    A. Agarwal, D. Karabali, and V. P. Nair, Fractional quantum hall effect in higher dimensions, Phys. Rev. D 111, 025002 (2025)

  80. [80]

    Ino and M

    K. Ino and M. Kohmoto, Critical properties of harper’s equation on a triangular lattice, Phys. Rev. B73, 205111 (2006)

Showing first 80 references.