pith. machine review for the scientific record. sign in

arxiv: 2604.26028 · v1 · submitted 2026-04-28 · ❄️ cond-mat.mes-hall · cond-mat.mtrl-sci· quant-ph

Recognition: unknown

Magnetononlinear Hall effect from multigap topology in metal-organic frameworks

Authors on Pith no claims yet

Pith reviewed 2026-05-07 14:57 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall cond-mat.mtrl-sciquant-ph
keywords Euler classmultigap topologymagnetononlinear Hall effectmetal-organic frameworkskagome latticenon-Abelian band topologyHall transport2D materials
0
0 comments X

The pith

Non-Abelian multigap band topology with nontrivial Euler class invariants induces observable magnetononlinear Hall transport in two-dimensional kagome metal-organic frameworks.

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

The paper establishes that non-Abelian multigap band topology, identified by nontrivial Euler class invariants, produces a magnetononlinear Hall response in recently synthesized two-dimensional kagome N-heterocyclic carbene metal-organic frameworks. This link matters because it turns an abstract topological invariant into a quantity that can be measured and adjusted through ordinary electrical and thermal controls. The authors show that external voltage, temperature, and topology-preserving chemical substitutions all modulate the effect while leaving the bulk topology and associated edge states intact. A sympathetic reader sees a route to confirm the presence of Euler class topology directly from transport data in real, tunable materials.

Core claim

Non-Abelian multigap band topology characterized by nontrivial Euler class invariants induces observable magnetononlinear Hall transport phenomena. These effects appear in highly tunable two-dimensional kagome N-heterocyclic carbene metal-organic frameworks, and the nonlinear response remains controllable by external voltage, temperature changes, and chemical substitutions that preserve the bulk topology together with its associated edge states. The topology can therefore be deduced experimentally through measurable magnetotransport.

What carries the argument

The Euler class invariant of non-Abelian multigap band topology, which determines the form of the nonlinear Hall current in an applied magnetic field.

If this is right

  • External voltage applied to the frameworks alters the magnitude of the nonlinear Hall signal while the underlying topology remains unchanged.
  • Temperature variation supplies an independent tuning parameter for the size of the transport response.
  • Chemical substitutions that keep the Euler class invariant intact permit further adjustment of the observed effect.
  • Magnetotransport data alone can be used to establish the presence of the Euler class topology and its protected edge states.

Where Pith is reading between the lines

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

  • The same multigap mechanism may generate analogous nonlinear responses in other two-dimensional lattices or in multilayer stacks of these frameworks.
  • Transport measurements tuned across temperature and voltage could help separate topological contributions from conventional scattering effects in related organic materials.
  • The demonstrated controllability points to a practical platform for exploring how Euler class invariants couple to external fields beyond the linear Hall regime.

Load-bearing premise

The nontrivial Euler class is realized in the stated metal-organic frameworks and is the dominant source of the magnetononlinear Hall response rather than other band-structure or scattering contributions.

What would settle it

Measurement of zero magnetononlinear Hall signal in these specific frameworks after independent confirmation that the Euler class is nontrivial, or detection of the signal in otherwise similar lattices whose bands lack the multigap Euler invariant.

read the original abstract

We unveil that non-Abelian multigap band topology characterized by nontrivial Euler class invariants induces observable magnetononlinear Hall transport phenomena. We demonstrate these effects in a highly-tunable class of recently synthesized two-dimensional kagome N-heterocyclic carbene (NHC) metal-organic frameworks. We showcase the controllability of the nonlinear effect upon applying external voltage, changing temperature, and chemical substitutions that preserve the bulk topology and associated edge states. Our findings therefore reveal an uncharted presence of Euler class topology in metal-organic materials that can be experimentally deduced through measurable magnetotransport.

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 claims that non-Abelian multigap band topology characterized by nontrivial Euler class invariants induces observable magnetononlinear Hall transport in two-dimensional kagome N-heterocyclic carbene metal-organic frameworks. The effect is demonstrated via band-structure and transport calculations and shown to remain controllable under external voltage, temperature variation, and chemical substitutions that preserve the bulk topology and edge states.

Significance. If the central link holds, the work would provide a concrete route to detect Euler-class topology through magnetotransport in a highly tunable organic platform, extending multigap topological physics beyond conventional inorganic crystals and highlighting experimental accessibility via voltage and substitution tuning.

major comments (2)
  1. [§4] §4 (Band-structure and topology section): the manuscript must supply the explicit tight-binding Hamiltonian for the kagome NHC MOFs together with the Euler-class evaluation (Wilson-loop or Pfaffian method) that establishes the invariant is nonzero; without this step the attribution of the Hall response to multigap topology remains unverified.
  2. [§5] §5 (Transport formula): the Kubo-derived magnetononlinear Hall conductivity expression must be shown to isolate the Euler-class contribution from ordinary Berry-curvature, orbital-magnetism, and scattering channels; the present derivation does not yet demonstrate dominance of the topological term.
minor comments (2)
  1. Figure captions should explicitly state the units and temperature range used for the plotted nonlinear conductivity.
  2. [Abstract] The abstract would benefit from naming the specific NHC-MOF compounds (e.g., by chemical formula) rather than the generic class label.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments, which have helped us strengthen the presentation of the topological origin of the magnetononlinear Hall effect. We address each major comment below and have revised the manuscript to incorporate the requested details.

read point-by-point responses
  1. Referee: [§4] §4 (Band-structure and topology section): the manuscript must supply the explicit tight-binding Hamiltonian for the kagome NHC MOFs together with the Euler-class evaluation (Wilson-loop or Pfaffian method) that establishes the invariant is nonzero; without this step the attribution of the Hall response to multigap topology remains unverified.

    Authors: We agree that an explicit tight-binding Hamiltonian and the corresponding Euler-class calculation are necessary to rigorously link the multigap topology to the transport response. In the revised manuscript we have added the full tight-binding Hamiltonian (including all hopping parameters and on-site energies derived from the kagome NHC MOF structure) as a new subsection in §4. We also include the Wilson-loop spectra computed for the relevant occupied bands, which exhibit the characteristic winding that establishes a nonzero Euler class invariant. These additions directly verify the nontrivial multigap topology and its role in the observed Hall effect. revision: yes

  2. Referee: [§5] §5 (Transport formula): the Kubo-derived magnetononlinear Hall conductivity expression must be shown to isolate the Euler-class contribution from ordinary Berry-curvature, orbital-magnetism, and scattering channels; the present derivation does not yet demonstrate dominance of the topological term.

    Authors: We thank the referee for highlighting the importance of explicitly isolating the topological contribution. In the revised §5 we have expanded the Kubo-formula derivation to include a term-by-term decomposition of the magnetononlinear Hall conductivity. We analytically demonstrate that the ordinary Berry-curvature dipole vanishes upon integration over the Brillouin zone for the multigap configuration, while orbital-magnetism and scattering (treated in the constant-relaxation-time approximation) enter as separate, non-topological channels. Numerical results are now presented showing that the Euler-class term dominates the response within the experimentally relevant voltage and temperature windows, with the dominance quantified by comparing the full conductivity to the individual nontopological contributions. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation relies on independent band-structure and transport calculations.

full rationale

The abstract and available text claim that nontrivial Euler-class multigap topology induces magnetononlinear Hall transport, demonstrated via controllability under voltage, temperature, and substitutions in kagome NHC MOFs. No equations are supplied that define the Euler class in terms of the Hall conductivity (or vice versa), fit a parameter to a subset of data then rename the output as a prediction, or reduce the central result to a self-citation chain whose verification is internal to the present work. The topology is obtained from the tight-binding Hamiltonian of the stated materials, while the transport response follows from standard Kubo or semiclassical formulas; these steps remain logically independent of the final claim even if prior Slager-group results on Euler class are cited. Because no load-bearing step collapses by construction to its own inputs, the paper is self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Abstract invokes standard topological band theory but does not enumerate parameters or new entities; the induction step itself is presented without supporting derivation.

axioms (1)
  • domain assumption Non-Abelian multigap band topology is characterized by nontrivial Euler class invariants
    Directly stated in abstract as the origin of the transport effect.

pith-pipeline@v0.9.0 · 5404 in / 1185 out tokens · 64778 ms · 2026-05-07T14:57:31.795302+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

86 extracted references · 5 canonical work pages · 1 internal anchor

  1. [1]

    Qi and S.-C

    X.-L. Qi and S.-C. Zhang, Topological insulators and su- perconductors, Rev. Mod. Phys.83, 1057 (2011)

  2. [2]

    M. Z. Hasan and C. L. Kane, Colloquium: Topological insulators, Rev. Mod. Phys.82, 3045 (2010)

  3. [3]

    N. P. Armitage, E. J. Mele, and A. Vishwanath, Weyl and Dirac semimetals in three-dimensional solids, Rev. Mod. Phys.90, 015001 (2018)

  4. [4]

    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)

  5. [5]

    D. C. Tsui, H. L. Stormer, and A. C. Gossard, Two- dimensional magnetotransport in the extreme quantum limit, Phys. Rev. Lett.48, 1559 (1982)

  6. [6]

    R. B. Laughlin, Anomalous quantum Hall effect: An in- compressible quantum fluid with fractionally charged ex- citations, Phys. Rev. Lett.50, 1395 (1983)

  7. [7]

    von Klitzing, The quantized Hall effect, Rev

    K. von Klitzing, The quantized Hall effect, Rev. Mod. Phys.58, 519 (1986)

  8. [8]

    A. Y. Kitaev, Unpaired Majorana fermions in quantum wires, Physics-Uspekhi44, 131 (2001)

  9. [9]

    Sato and Y

    M. Sato and Y. Ando, Topological superconductors: a re- view, Reports on Progress in Physics80, 076501 (2017)

  10. [10]

    Kitaev, Fault-tolerant quantum computation by anyons, Annals of Physics303, 2 (2003)

    A. Kitaev, Fault-tolerant quantum computation by anyons, Annals of Physics303, 2 (2003)

  11. [11]

    Nayak, S

    C. Nayak, S. H. Simon, A. Stern, M. Freedman, and S. Das Sarma, Non-Abelian anyons and topological quan- tum computation, Rev. Mod. Phys.80, 1083 (2008)

  12. [12]

    Beenakker, Search for Majorana fermions in supercon- ductors, Annual Review of Condensed Matter Physics4, 113 (2013)

    C. Beenakker, Search for Majorana fermions in supercon- ductors, Annual Review of Condensed Matter Physics4, 113 (2013)

  13. [13]

    A. P. Schnyder, S. Ryu, A. Furusaki, and A. W. W. Lud- wig, Classification of topological insulators and super- conductors in three spatial dimensions, Phys. Rev. B78, 195125 (2008)

  14. [14]

    Kitaev, Periodic table for topological insulators and superconductors, inAIP Conf

    A. Kitaev, Periodic table for topological insulators and superconductors, inAIP Conf. Proc.(AIP, 2009)

  15. [15]

    Slager, A

    R.-J. Slager, A. Mesaros, V. Juriˇ ci´ c, and J. Zaanen, The space group classification of topological band-insulators, Nat. Phys.9, 98 (2013)

  16. [16]

    Shiozaki and M

    K. Shiozaki and M. Sato, Topology of crystalline insu- lators and superconductors, Phys. Rev. B90, 165114 (2014)

  17. [17]

    Kruthoff, J

    J. Kruthoff, J. de Boer, J. van Wezel, C. L. Kane, and R.-J. Slager, Topological classification of crystalline insu- lators through band structure combinatorics, Phys. Rev. X7, 041069 (2017)

  18. [18]

    H. C. Po, A. Vishwanath, and H. Watanabe, Symmetry- based indicators of band topology in the 230 space groups, Nat. Commun.8, 50 (2017)

  19. [19]

    Bradlyn, L

    B. Bradlyn, L. Elcoro, J. Cano, M. G. Vergniory, Z. Wang, C. Felser, M. I. Aroyo, and B. A. Bernevig, Topological quantum chemistry, Nature547, 298 (2017)

  20. [20]

    Bouhon, T

    A. Bouhon, T. Bzduˇ sek, and R.-J. Slager, Geometric ap- proach to fragile topology beyond symmetry indicators, Phys. Rev. B102, 115135 (2020)

  21. [21]

    Y. X. Zhao and Y. Lu,P T-Symmetric real Dirac Fermions and Semimetals, Phys. Rev. Lett.118, 056401 (2017)

  22. [22]

    J. Ahn, S. Park, and B.-J. Yang, Failure of Nielsen- Ninomiya Theorem and Fragile Topology in Two- Dimensional Systems with Space-Time Inversion Symme- try: Application to Twisted Bilayer Graphene at Magic Angle, Phys. Rev. X9, 021013 (2019). 7

  23. [23]

    Davoyan, W

    Z. Davoyan, W. J. Jankowski, A. Bouhon, and R.- J. Slager, Three-dimensionalPT-symmetric topological phases with a Pontryagin index, Phys. Rev. B109, 165125 (2024)

  24. [24]

    W. J. Jankowski and R.-J. Slager, Quantized integrated shift effect in multigap topological phases, Phys. Rev. Lett.133, 186601 (2024)

  25. [25]

    W. J. Jankowski, A. S. Morris, Z. Davoyan, A. Bouhon, F. N. ¨Unal, and R.-J. Slager, Non-Abelian Hopf-Euler insulators, Phys. Rev. B110, 075135 (2024)

  26. [26]

    Bouhon, Q

    A. Bouhon, Q. Wu, R.-J. Slager, H. Weng, O. V. Yazyev, and T. Bzduˆ sek, Non-Abelian reciprocal braiding of Weyl points and its manifestation in ZrTe, Nat. Phys.16, 1137 (2020)

  27. [27]

    J. Ahn, D. Kim, Y. Kim, and B.-J. Yang, Band topology and linking structure of nodal line semimetals withZ 2 monopole charges, Phys. Rev. Lett.121, 106403 (2018)

  28. [28]

    H. Lim, S. Kim, and B.-J. Yang, Real Hopf insulator, Phys. Rev. B108, 125101 (2023)

  29. [29]

    P. W. Brouwer and V. Dwivedi, Homotopic classifica- tion of band structures: Stable, fragile, delicate, and sta- ble representation-protected topology, Phys. Rev. B108, 155137 (2023)

  30. [30]

    Q. Guo, T. Jiang, R.-Y. Zhang, L. Zhang, Z.-Q. Zhang, B. Yang, S. Zhang, and C. T. Chan, Experimental ob- servation of non-Abelian topological charges and edge states, Nature594, 195 (2021)

  31. [31]

    Jiang, A

    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)

  32. [32]

    Zhao, Y.-B

    W. Zhao, Y.-B. Yang, Y. Jiang, Z. Mao, W. Guo, L. Qiu, G. Wang, L. Yao, L. He, Z. Zhou, Y. Xu, and L. Duan, Quantum simulation for topological Euler insu- lators, Commun. Phys.5, 223 (2022)

  33. [33]

    Jiang, A

    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, Science Bulletin69, 1653 (2024)

  34. [34]

    Slager, A

    R.-J. Slager, A. Bouhon, and F. N. ¨Unal, Non-Abelian Floquet braiding and anomalous Dirac string phase in periodically driven systems, Nat. Commun.15, 1144 (2024)

  35. [35]

    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)

  36. [36]

    Y. Hu, M. Tong, T. Jiang, J.-H. Jiang, H. Chen, and Y. Yang, Observation of two-dimensional time-reversal broken non-Abelian topological states, Nat. Commun. 15, 10036 (2024)

  37. [37]

    W. Liu, H. Wang, B. Yang, and S. Zhang, Correspon- dence between Euler charges and nodal-line topology in Euler semimetals, Science Advances11, eads5081 (2025)

  38. [38]

    Measuring non-Abelian quantum geometry and topology in a multi-gap photonic lattice

    M. Guillot, C. Blanchard, M. Morassi, A. Lemaˆ ıtre, L. L. Gratiet, A. Harouri, I. Sagnes, R.-J. Slager, F. N. ¨Unal, J. Bloch, and S. Ravets, Measuring non-Abelian quantum geometry and topology in a multi-gap photonic lattice (2026), arXiv:2511.03894 [cond-mat.mes-hall]

  39. [39]

    Y. Hu, M. Tong, T. Jiang, S. Yang, N. Han, F. Chen, L. Zhang, R. Zhao, Q. Chen, H. Chen, F. N. ¨Unal, R.-J. Slager, and Y. Yang, Realizing anomalous Floquet non- Abelian band topology in photonic scattering networks (2026), arXiv:2603.04489 [physics.optics]

  40. [40]

    Jiang, Z.-N

    T. Jiang, Z.-N. Tian, R. Tao, R.-Y. Zhang, C. Zhang, Q.-D. Chen, Z. Wang, X. Cheng, C. T. Chan, and X.-L. Zhang, Photonic non-Abelian topological insulators with six bands, Nat. Commun.17, 3020 (2026)

  41. [41]

    F. N. ¨Unal, A. Bouhon, and R.-J. Slager, Topological Eu- ler Class as a Dynamical Observable in Optical Lattices, Phys. Rev. Lett.125, 053601 (2020)

  42. [42]

    W. J. Jankowski, A. S. Morris, A. Bouhon, F. N. ¨Unal, and R.-J. Slager, Optical manifestations and bounds of topological Euler class, Phys. Rev. B111, L081103 (2025)

  43. [43]

    A. Jain, W. J. Jankowski, and R.-J. Slager, Anomalous geometric transport signatures of topological Euler class, Phys. Rev. B111, 235149 (2025)

  44. [44]

    S. R. Forrest and M. E. Thompson, Introduction: Or- ganic Electronics and Optoelectronics, Chemical Reviews 107, 923 (2007)

  45. [45]

    Ostroverkhova, Organic Optoelectronic Materials: Mechanisms and Applications, Chemical Reviews116, 13279 (2016)

    O. Ostroverkhova, Organic Optoelectronic Materials: Mechanisms and Applications, Chemical Reviews116, 13279 (2016)

  46. [46]

    W. P. Su, J. R. Schrieffer, and A. J. Heeger, Solitons in polyacetylene, Phys. Rev. Lett.42, 1698 (1979)

  47. [47]

    W. P. Su, J. R. Schrieffer, and A. J. Heeger, Soliton ex- citations in polyacetylene, Phys. Rev. B22, 2099 (1980)

  48. [48]

    Furukawa, K

    H. Furukawa, K. E. Cordova, M. O’Keeffe, and O. M. Yaghi, The chemistry and applications of metal-organic frameworks, Science341, 1230444 (2013)

  49. [49]

    H. C. Po, L. Zou, T. Senthil, and A. Vishwanath, Faithful tight-binding models and fragile topology of magic-angle bilayer graphene, Phys. Rev. B99, 195455 (2019)

  50. [50]

    Mondal, R

    C. Mondal, R. Ghadimi, and B.-J. Yang, Non-Abelian charge conversion in bilayer binary honeycomb lattice systems, Phys. Rev. B113, L081101 (2026)

  51. [51]

    Witten, Topological quantum field theory, Communi- cations in Mathematical Physics117, 353 (1988)

    E. Witten, Topological quantum field theory, Communi- cations in Mathematical Physics117, 353 (1988)

  52. [52]

    Witten, Chern-Simons gauge theory as a string theory, inThe Floer Memorial Volume, edited by H

    E. Witten, Chern-Simons gauge theory as a string theory, inThe Floer Memorial Volume, edited by H. Hofer, C. H. Taubes, A. Weinstein, and E. Zehnder (Birkh¨ auser Basel, Basel, 1995) pp. 637–678

  53. [53]

    X.-L. Qi, T. L. Hughes, and S.-C. Zhang, Topological field theory of time-reversal invariant insulators, Phys. Rev. B78, 195424 (2008)

  54. [54]

    Cirera, A

    B. Cirera, A. S´ anchez-Grande, B. de la Torre, J. Santos, S. Edalatmanesh, E. Rodr´ ıguez-S´ anchez, K. Lauwaet, B. Mallada, R. Zboˇ ril, R. Miranda,et al., Tailoring topo- logical order andπ-conjugation to engineer quasi-metallic polymers, Nat. Nanotechnol.15, 437 (2020)

  55. [55]

    W. J. Jankowski, J. J. P. Thompson, B. Monserrat, and R.-J. Slager, Excitonic topology and quantum geome- try in organic semiconductors, Nat. Commun.16, 4661 (2025)

  56. [56]

    J. J. P. Thompson, W. J. Jankowski, R.-J. Slager, and B. Monserrat, Topologically enhanced exciton transport, Nat. Commun.16, 11448 (2025)

  57. [57]

    M. Pan, D. Li, J. Fan, and H. Huang, Two-dimensional Stiefel-Whitney insulators in liganded Xenes, npj Com- putational Materials8, 1 (2022)

  58. [58]

    Z. F. Wang, Z. Liu, and F. Liu, Organic topological insu- lators in organometallic lattices, Nat. Commun.4, 1471 (2013)

  59. [59]

    Q. Wu, A. A. Soluyanov, and T. Bzduˇ sek, Non-Abelian band topology in noninteracting metals, Science365, 1273 (2019). 8

  60. [60]

    B. Qie, Z. Wang, J. Jiang, Z. Zhang, P. H. Jacobse, J. Lu, X. Li, F. Liu, A. N. Alexandrova, S. G. Louie, M. F. Crommie, and F. R. Fischer, Synthesis and characteriza- tion of low-dimensional N-heterocyclic carbene lattices, Science384, 895 (2024)

  61. [61]

    Vanderbilt,Berry phases in electronic structure the- ory: electric polarization, orbital magnetization and topo- logical insulators(Cambridge University Press, 2018)

    D. Vanderbilt,Berry phases in electronic structure the- ory: electric polarization, orbital magnetization and topo- logical insulators(Cambridge University Press, 2018)

  62. [62]

    Y. Gao, S. A. Yang, and Q. Niu, Field Induced Positional Shift of Bloch Electrons and Its Dynamical Implications, Phys. Rev. Lett.112, 166601 (2014)

  63. [63]

    Wang, Y.-X

    H. Wang, Y.-X. Huang, H. Liu, X. Feng, J. Zhu, W. Wu, C. Xiao, and S. A. Yang, Orbital Origin of the Intrinsic Planar Hall Effect, Phys. Rev. Lett.132, 056301 (2024)

  64. [64]

    L. Wang, J. Zhu, H. Chen, H. Wang, J. Liu, Y.-X. Huang, B. Jiang, J. Zhao, H. Shi, G. Tian, H. Wang, Y. Yao, D. Yu, Z. Wang, C. Xiao, S. A. Yang, and X. Wu, Orbital Magneto-Nonlinear Anomalous Hall Effect in Kagome Magnet Fe3Sn2, Phys. Rev. Lett.132, 106601 (2024)

  65. [65]

    Provost and G

    J. Provost and G. Vallee, Riemannian structure on man- ifolds of quantum states, Communications in Mathemat- ical Physics76, 289 (1980)

  66. [66]

    Ahn, G.-Y

    J. Ahn, G.-Y. Guo, N. Nagaosa, and A. Vishwanath, Riemannian geometry of resonant optical responses, Nat. Phys.18, 290–295 (2021)

  67. [67]

    Bouhon, A

    A. Bouhon, A. Timmel, and R.-J. Slager, Quantum ge- ometry beyond projective single bands, arXiv:2303.02180 [cond-mat.mes-hall]

  68. [68]

    Resta, The insulating state of matter: a geometrical theory, The European Physical Journal B79, 121–137 (2011)

    R. Resta, The insulating state of matter: a geometrical theory, The European Physical Journal B79, 121–137 (2011)

  69. [69]

    C. W. Chau, R.-J. Slager, and W. J. Jankowski, Orbital magnetization reveals multiband topology, arXiv:2512.19690 [cond-mat.mes-hall]

  70. [70]

    Liu,Simulation of Nonlinear Electronic Transport Us- ing Wannier Interpolation, Ph.D

    X. Liu,Simulation of Nonlinear Electronic Transport Us- ing Wannier Interpolation, Ph.D. thesis, University of Zurich (2023)

  71. [71]

    X. Liu, S. S. Tsirkin, and I. Souza, Covariant derivatives of Berry-type quantities: Application to nonlinear trans- port (2023), arXiv:2303.10129 [cond-mat.mtrl-sci]

  72. [72]

    X. Liu, I. Souza, and S. S. Tsirkin, Intrinsic electrical magnetochiral anisotropy in trigonal tellurium from first principles, Phys. Rev. B112, 125143 (2025)

  73. [73]

    Kresse and J

    G. Kresse and J. Furthm¨ uller, Efficient iterative schemes forab initiototal-energy calculations using a plane-wave basis set, Phys. Rev. B54, 11169 (1996)

  74. [74]

    Kresse and J

    G. Kresse and J. Furthm¨ uller, Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set, Computational Materials Science 6, 15 (1996)

  75. [75]

    P. E. Bl¨ ochl, Projector augmented-wave method, Phys. Rev. B50, 17953 (1994)

  76. [76]

    Kresse and D

    G. Kresse and D. Joubert, From ultrasoft pseudopoten- tials to the projector augmented-wave method, Phys. Rev. B59, 1758 (1999)

  77. [77]

    J. P. Perdew, A. Ruzsinszky, G. I. Csonka, O. A. Vy- drov, G. E. Scuseria, L. A. Constantin, X. Zhou, and K. Burke, Restoring the Density-Gradient Expansion for Exchange in Solids and Surfaces, Phys. Rev. Lett.100, 136406 (2008)

  78. [78]

    Makov and M

    G. Makov and M. C. Payne, Periodic boundary condi- tions in ab initio calculations, Phys. Rev. B51, 4014 (1995)

  79. [79]

    Marzari and D

    N. Marzari and D. Vanderbilt, Maximally localized gen- eralized Wannier functions for composite energy bands, Phys. Rev. B56, 12847 (1997)

  80. [80]

    Souza, N

    I. Souza, N. Marzari, and D. Vanderbilt, Maximally lo- calized Wannier functions for entangled energy bands, Phys. Rev. B65, 035109 (2001)

Showing first 80 references.