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arxiv: 2605.14349 · v1 · submitted 2026-05-14 · ❄️ cond-mat.dis-nn · cond-mat.mes-hall

Recognition: 2 theorem links

· Lean Theorem

Quantum Criticality in Monolayer Amorphous Carbon

Authors on Pith no claims yet

Pith reviewed 2026-05-15 01:58 UTC · model grok-4.3

classification ❄️ cond-mat.dis-nn cond-mat.mes-hall
keywords monolayer amorphous carbonAnderson criticalitytopological disordermultifractal wavefunctionsWess-Zumino-Witten termchiral symmetry2D amorphous systems
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The pith

Monolayer amorphous carbon exhibits Anderson criticality at the band center driven purely by topological disorder.

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

The paper examines electronic states in monolayer amorphous carbon, a strictly two-dimensional material formed by a topologically disordered sp2-bonded random network with no long-range order. Atomic-resolution measurements show that this disorder localizes most low-energy electronic states while preserving an extended critical-like state near zero energy. The authors conjecture that remnant chiral symmetry within the network protects this state, described by a Wess-Zumino-Witten topological term. They verify the associated multifractal scaling relation between spatial correlations and scaling exponents, with matching results from tight-binding calculations. This positions MAC as the first strictly 2D amorphous system displaying Anderson criticality from topological disorder alone.

Core claim

In monolayer amorphous carbon, topological disorder in the sp2-bonded random network localizes electronic states away from the band center but preserves an extended critical state near E~0, protected by remnant chiral symmetry via a Wess-Zumino-Witten term. Atomic-resolution measurements of multifractal wavefunctions confirm the scaling relation η = -Δ₂ with quantitative agreement to spatial correlation decay, and atomistic tight-binding calculations reproduce the multifractal scaling near E~0. These results establish MAC as the first strictly 2D amorphous electronic system to exhibit Anderson criticality driven purely by topological disorder.

What carries the argument

The Wess-Zumino-Witten topological term that encodes protection of the critical state at E~0 by remnant chiral symmetry surviving in the continuous random network.

If this is right

  • The critical state near E=0 displays multifractal scaling with the relation η = -Δ₂ matching independent measurements of spatial correlation decay.
  • Atomistic tight-binding calculations closely reproduce the experimental multifractal scaling near the band center.
  • Topological disorder alone, without crystalline order or additional symmetry breaking, suffices to produce Anderson criticality in a strictly 2D amorphous lattice.
  • MAC provides a concrete realization for studying quantum critical phenomena in two-dimensional systems defined solely by a continuous random network.

Where Pith is reading between the lines

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

  • Similar critical states protected by remnant symmetries could appear in other 2D amorphous sp2 networks if the chiral protection mechanism generalizes.
  • Introducing controlled symmetry-breaking defects would allow direct tests of whether the critical state disappears as predicted.
  • The result opens routes to engineer quantum critical points in disordered 2D carbon materials for potential electronic applications.

Load-bearing premise

The critical state near zero energy remains protected from topological disorder by a remnant chiral symmetry that survives in the continuous random network and is described by a Wess-Zumino-Witten term.

What would settle it

Observation that the extended critical state or its multifractal scaling near E=0 vanishes when a controlled perturbation explicitly breaks the remnant chiral symmetry would falsify the proposed protection mechanism.

Figures

Figures reproduced from arXiv: 2605.14349 by Abee Nelson, Arsen Herasymchuk, Artem K Grebenko, Barbaros Ozyilmaz, Bent Weber, Chee Tat Toh, Gagandeep Singh, Hanning Zhang, Hongji Zhang, Kazutomo Suenaga, Naoto Kimiuchi, Oleg V. Yazyev, Ranjith Shivajirao, Rejaul Sk, Rudolf A Romer, Shaffique Adam, Yuta Sato, Zheng Jue Tong.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: c). This is distinctly different from the behavior at higher energies, where the correlation length decays rapidly. The theoretical description of critical wavefunctions predicts that spatial correlations are linked to multifrac￾tality through the scaling relation η = −∆2 [4]. We extract the power-law decay exponent of the spatial cor￾relation η at all energies (Fig. 3b) and compared it vis￾a-vis with the … view at source ↗
read the original abstract

Amorphous solids represent the extreme limit of broken translational symmetry, in which the absence of long-range order removes well-defined crystal momenta and invalidates the Bloch description of electronic states. Monolayer amorphous carbon (MAC) has emerged as a unique realization of a strictly two-dimensional (2D) amorphous lattice defined by a structurally contiguous but topologically disordered $sp^2$-bonded random network devoid of any defined long-range crystal symmetry. From atomic-resolution measurements of multifractal wavefunctions, we show that disorder in MAC effectively localizes the low-energy part of the electronic spectrum but retains an extended critical-like state near the band centre ($E\sim 0$). We conjecture that this state is protected from topological disorder by remnant chiral symmetry surviving within the continuous random network, described by a Wess-Zumino-Witten (WZW) topological term. Near criticality, we verify the multifractal scaling relation $\eta = -\Delta_2$, providing quantitative agreement between independently measured spatial correlation decay and multifractal scaling exponents. Our results are confirmed by atomistic tight-binding calculations that closely mirror the multifractal scaling near $E\sim 0$. Our results establish MAC as the first strictly 2D amorphous electronic system to exhibit Anderson criticality driven purely by topological disorder

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 / 1 minor

Summary. The manuscript reports atomic-resolution measurements of multifractal wavefunctions in monolayer amorphous carbon (MAC), a strictly 2D sp²-bonded random network, together with atomistic tight-binding calculations. It claims that topological disorder localizes most of the spectrum but leaves an extended critical state near E=0, conjectured to be protected by remnant chiral symmetry described by a Wess-Zumino-Witten term; the multifractal scaling relation η = −Δ₂ is verified by independent spatial-correlation and scaling-exponent measurements, establishing MAC as the first strictly 2D amorphous system exhibiting Anderson criticality driven purely by topological disorder.

Significance. If the central conjecture is substantiated, the work would identify a new, experimentally accessible platform for Anderson criticality in two dimensions without crystalline order or external fields, with quantitative agreement between measured and calculated multifractal exponents providing a concrete benchmark for theories of disordered 2D systems.

major comments (2)
  1. [Abstract] Abstract and summary: the claim that the critical state near E=0 is protected by remnant chiral symmetry (via a WZW term) is presented as a conjecture without ring-statistics data, without an explicit check that the tight-binding Hamiltonian anticommutes with a chiral operator, and without a derivation showing why the effective theory remains WZW rather than gapped or localized once bipartiteness is lost.
  2. [Summary] The reported multifractal scaling η = −Δ₂, while consistent between experiment and calculation, does not by itself establish the symmetry class or rule out conventional 2D Anderson localization; an independent diagnostic (e.g., level statistics or explicit chiral-operator test) is required to support the topological-protection interpretation.
minor comments (1)
  1. [Abstract] Clarify in the abstract whether the WZW term is fitted to data or invoked on symmetry grounds alone.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed comments, which have helped clarify several aspects of our presentation. We respond to each major comment below and indicate the revisions we will make.

read point-by-point responses
  1. Referee: [Abstract] Abstract and summary: the claim that the critical state near E=0 is protected by remnant chiral symmetry (via a WZW term) is presented as a conjecture without ring-statistics data, without an explicit check that the tight-binding Hamiltonian anticommutes with a chiral operator, and without a derivation showing why the effective theory remains WZW rather than gapped or localized once bipartiteness is lost.

    Authors: We agree that the protection mechanism is presented as a conjecture, as a full microscopic derivation of the effective WZW theory lies beyond the scope of the present experimental and computational study. The tight-binding calculations are performed on the experimentally determined atomic coordinates, which directly encode the ring statistics of the continuous random network. In the revised manuscript we will add (i) an explicit numerical verification that the Hamiltonian anticommutes with a chiral operator defined on the two sublattices (even in the presence of odd-membered rings) and (ii) a concise outline in the supplementary information of the effective-field-theory argument for the survival of the WZW term. We will also include a brief quantitative summary of the ring-size distribution extracted from the atomic-resolution images. revision: partial

  2. Referee: [Summary] The reported multifractal scaling η = −Δ₂, while consistent between experiment and calculation, does not by itself establish the symmetry class or rule out conventional 2D Anderson localization; an independent diagnostic (e.g., level statistics or explicit chiral-operator test) is required to support the topological-protection interpretation.

    Authors: We accept that the scaling relation alone does not uniquely determine the symmetry class. The supporting evidence in the manuscript is the quantitative agreement between measured and calculated multifractal exponents together with the fact that localization occurs away from E=0 while criticality persists at the band center. To strengthen the interpretation we will add, in the revised version, (i) the nearest-neighbor level-spacing distribution near E=0, which shows the linear repulsion characteristic of the chiral orthogonal ensemble, and (ii) the explicit chiral-operator anticommutation test already mentioned above. These diagnostics will be presented alongside the existing multifractal analysis. revision: yes

Circularity Check

0 steps flagged

No load-bearing circularity; multifractal verification independent and WZW presented as conjecture

full rationale

The central result rests on direct spatial measurements of wavefunction correlations and multifractal exponents that are cross-checked against each other and against independent tight-binding numerics; these steps do not reduce to a fitted parameter renamed as a prediction. The WZW protection is explicitly labeled a conjecture rather than derived from the data or from a self-citation chain. The 'first strictly 2D' claim is a literature-survey statement, not an internal derivation. No equation or section shows a self-definitional loop or a uniqueness theorem imported from the same authors' prior work that would force the conclusion.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on remnant chiral symmetry in the random network and the applicability of the WZW topological term; no free parameters are explicitly fitted in the abstract, and no new particles or dimensions are introduced.

axioms (2)
  • domain assumption Remnant chiral symmetry survives within the continuous random network of MAC
    Invoked to protect the critical state near E=0 from topological disorder
  • domain assumption The critical state is described by a Wess-Zumino-Witten topological term
    Conjectured to explain protection from disorder

pith-pipeline@v0.9.0 · 5615 in / 1427 out tokens · 33446 ms · 2026-05-15T01:58:44.969564+00:00 · methodology

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Reference graph

Works this paper leans on

64 extracted references · 64 canonical work pages

  1. [1]

    Here, we apply the same tech- nique to probe the criticality in a strictly 2D amorphous material

    disordered systems. Here, we apply the same tech- nique to probe the criticality in a strictly 2D amorphous material. For the first time, here we tie electronic wave func- tion structure and response to microscopically resolved topological lattice disorder of MAC as a truly 2D amor- phous monolayer. Using STM and STS, we observe mul- tifractal scaling [38...

  2. [2]

    ‘Quantum Geometric Advantage’. VII. AUTHOR CONTRIBUTIONS RSK performed the scanning tunnelling microscopy and spectroscopy experiments with help from RS GS and ZJT. AKG CTT and HZ prepared the MAC samples. RSK and BW analyzed the STM/STS data. RSK per- formed the multifractal analysis with the help of BW, RS and AN. NK, YS and KS performed the TEM exper- ...

  3. [3]

    Kramer and A

    B. Kramer and A. MacKinnon, Localization: theory and experiment, Reports on Progress in Physics56, 1469 (1993)

  4. [4]

    P. W. Anderson, Absence of Diffusion in Certain Random Lattices, Physical Review109, 1492 (1958)

  5. [5]

    Abrahams, P

    E. Abrahams, P. W. Anderson, D. C. Licciardello, and T. V. Ramakrishnan, Scaling Theory of Localization: Absence of Quantum Diffusion in Two Dimensions, Phys- ical Review Letters42, 673 (1979)

  6. [6]

    Evers and A

    F. Evers and A. D. Mirlin, Anderson transitions, Reviews of Modern Physics80, 1355 (2008)

  7. [7]

    Billy, V

    J. Billy, V. Josse, Z. Zuo, A. Bernard, B. Hambrecht, P. Lugan, D. Cl´ ement, L. Sanchez-Palencia, P. Bouyer, and A. Aspect, Direct observation of Anderson localiza- tion of matter waves in a controlled disorder, Nature453, 891 (2008)

  8. [8]

    Roati, C

    G. Roati, C. D’Errico, L. Fallani, M. Fattori, C. Fort, M. Zaccanti, G. Modugno, M. Modugno, and M. In- guscio, Anderson localization of a non-interacting Bose–Einstein condensate, Nature453, 895 (2008)

  9. [9]

    Deissler, M

    B. Deissler, M. Zaccanti, G. Roati, C. D’Errico, M. Fat- tori, M. Modugno, G. Modugno, and M. Inguscio, De- localization of a disordered bosonic system by repulsive interactions, Nature Physics6, 354 (2010)

  10. [10]

    Segev, Y

    M. Segev, Y. Silberberg, and D. N. Christodoulides, An- derson localization of light, Nature Photonics7, 197 (2013)

  11. [11]

    A. B. Khanikaev, S. Hossein Mousavi, W.-K. Tse, M. Kargarian, A. H. MacDonald, and G. Shvets, Pho- tonic topological insulators, Nature Materials12, 233 (2013)

  12. [12]

    Sapienza, H

    L. Sapienza, H. Thyrrestrup, S. Stobbe, P. D. Garcia, S. Smolka, and P. Lodahl, Cavity Quantum Electrody- namics with Anderson-Localized Modes, Science327, 1352 (2010)

  13. [13]

    Schwartz, G

    T. Schwartz, G. Bartal, S. Fishman, and M. Segev, Transport and Anderson localization in disordered two- dimensional photonic lattices, Nature446, 52 (2007). 8

  14. [14]

    H. Hu, A. Strybulevych, J. H. Page, S. E. Skipetrov, and B. A. van Tiggelen, Localization of ultrasound in a three-dimensional elastic network, Nature Physics4, 945 (2008)

  15. [15]

    Malavi and S

    P. Malavi and S. Karmakar, Enhancement of Su- perconductivity by Anderson Localization in Three- Dimensional Crystalline Phase of BiSe, Physical Review Letters134, 196001 (2025)

  16. [16]

    K. Zhao, H. Lin, X. Xiao, W. Huang, W. Yao, M. Yan, Y. Xing, Q. Zhang, Z.-X. Li, S. Hoshino, J. Wang, S. Zhou, L. Gu, M. S. Bahramy, H. Yao, N. Nagaosa, Q.-K. Xue, K. T. Law, X. Chen, and S.-H. Ji, Disorder- induced multifractal superconductivity in monolayer nio- bium dichalcogenides, Nature Physics15, 904 (2019)

  17. [17]

    Li, R.-L

    J. Li, R.-L. Chu, J. K. Jain, and S.-Q. Shen, Topological Anderson Insulator, Physical Review Letters102, 136806 (2009)

  18. [18]

    E. J. Meier, F. A. An, A. Dauphin, M. Maffei, P. Massig- nan, T. L. Hughes, and B. Gadway, Observation of the topological Anderson insulator in disordered atomic wires, Science362, 929 (2018)

  19. [19]

    Zhang, D

    W. Zhang, D. Zou, Q. Pei, W. He, J. Bao, H. Sun, and X. Zhang, Experimental Observation of Higher-Order Topological Anderson Insulators, Physical Review Let- ters126, 146802 (2021)

  20. [20]

    Altland and M

    A. Altland and M. R. Zirnbauer, Nonstandard symme- try classes in mesoscopic normal-superconducting hybrid structures, Physical Review B55, 1142 (1997)

  21. [21]

    S. Ryu, C. Mudry, H. Obuse, and A. Furusaki, Z 2 topological term, the global anomaly, and the two- dimensional symplectic symmetry class of anderson lo- calization, Physical Review Letters99, 116601 (2007)

  22. [22]

    Punnoose and A

    A. Punnoose and A. M. Finkel’stein, Metal-Insulator Transition in Disordered Two-Dimensional Electron Sys- tems, Science310, 289 (2005)

  23. [23]

    Das Sarma, S

    S. Das Sarma, S. Adam, E. H. Hwang, and E. Rossi, Elec- tronic transport in two-dimensional graphene, Reviews of Modern Physics83, 407 (2011)

  24. [24]

    J. H. Garc´ ıa, B. Uchoa, L. Covaci, and T. G. Rappoport, Adatoms and Anderson localization in graphene, Physi- cal Review B90, 085425 (2014)

  25. [25]

    Z. Fan, A. Uppstu, and A. Harju, Anderson localiza- tion in two-dimensional graphene with short-range disor- der: One-parameter scaling and finite-size effects, Phys- ical Review B89, 245422 (2014)

  26. [26]

    Xiong and Y

    S.-J. Xiong and Y. Xiong, Anderson localization of elec- tron states in graphene in different types of disorder, Physical Review B76, 214204 (2007)

  27. [27]

    Gonz´ alez-Santander, F

    C. Gonz´ alez-Santander, F. Dom´ ınguez-Adame, M. Hilke, and R. A. R¨ omer, Localisation and finite-size effects in graphene flakes, Europhysics Letters104, 17012 (2013)

  28. [28]

    Street,Hydrogenated Amorphous Silicon, Cambridge Solid State Science Series (Cambridge University Press, 1991)

    R. Street,Hydrogenated Amorphous Silicon, Cambridge Solid State Science Series (Cambridge University Press, 1991)

  29. [29]

    X. Liu, D. R. Queen, T. H. Metcalf, J. E. Karel, and F. Hellman, Hydrogen-free amorphous silicon with no tunneling states, Physical review letters113, 025503 (2014)

  30. [30]

    Yaglioglu, H

    B. Yaglioglu, H. Yeom, R. Beresford, and D. C. Paine, High-mobility amorphous in2o3–10wt% zno thin film transistors, Applied Physics Letters89(2006)

  31. [31]

    Jankousky, D

    M. Jankousky, D. Pashov, J. H. Mazo, R. E. Larsen, V. Dobrosavljevi´ c, M. van Schilfgaarde, and V. Ste- vanovi´ c, Effective bands and band-like electron transport in amorphous solids, Nature Physics22, 88 (2026)

  32. [32]

    Corbae, S

    P. Corbae, S. Ciocys, D. Varjas, E. Kennedy, S. Zelt- mann, M. Molina-Ruiz, S. M. Griffin, C. Jozwiak, Z. Chen, L.-W. Wang, A. M. Minor, M. Scott, A. G. Grushin, A. Lanzara, and F. Hellman, Observation of spin-momentum locked surface states in amorphous Bi2Se3, Nature Materials22, 200 (2023)

  33. [33]

    Corbae, J

    P. Corbae, J. D. Hannukainen, Q. Marsal, D. Mu˜ noz- Segovia, and A. G. Grushin, Amorphous topological mat- ter: Theory and experiment, Europhysics Letters142, 16001 (2023)

  34. [34]

    Van Tuan, A

    D. Van Tuan, A. Kumar, S. Roche, F. Ortmann, M. Thorpe, and P. Ordejon, Insulating behavior of an amorphous graphene membrane, Physical Review B—Condensed Matter and Materials Physics86, 121408 (2012)

  35. [35]

    G. T. Barkema and N. Mousseau, High-quality contin- uous random networks, Physical Review B62, 4985 (2000)

  36. [36]

    Grimm, R

    U. Grimm, R. R¨ omer, and G. Schliecker, Electronic states in topologically disordered systems, Annalen der Physik 510, 389 (1998)

  37. [37]

    Bhattacharjee, P

    S. Bhattacharjee, P. Sierant, M. Dudy´ nski, J. Wehr, J. Zakrzewski, and M. Lewenstein, Anderson localization induced by structural disorder, Physical Review B111, L180202 (2025)

  38. [38]

    C.-T. Toh, H. Zhang, J. Lin, A. S. Mayorov, Y.-P. Wang, C. M. Orofeo, D. B. Ferry, H. Andersen, N. Kakenov, Z. Guo, I. H. Abidi, H. Sims, K. Suenaga, S. T. Pan- telides, and B. ¨Ozyilmaz, Synthesis and properties of free- standing monolayer amorphous carbon, Nature577, 199 (2020)

  39. [39]

    X. Bai, P. Hu, A. Li, Y. Zhang, A. Li, G. Zhang, Y. Xue, T. Jiang, Z. Wang, H. Cui, J. Kang, H. Zhao, L. Gu, W. Zhou, L.-M. Liu, X. Qiu, and L. Guo, Nitrogen-doped amorphous monolayer carbon, Nature634, 80 (2024)

  40. [40]

    Richardella, P

    A. Richardella, P. Roushan, S. Mack, B. Zhou, D. A. Huse, D. D. Awschalom, and A. Yazdani, Visualizing Critical Correlations Near the Metal-Insulator Transition in Ga1-xMnxAs, Science 10.1126/science.1183640 (2010)

  41. [41]

    J¨ ack, F

    B. J¨ ack, F. Zinser, E. J. K¨ onig, S. N. P. Wissing, A. B. Schmidt, M. Donath, K. Kern, and C. R. Ast, Visualiz- ing the multifractal wave functions of a disordered two- dimensional electron gas, Physical Review Research3, 013022 (2021)

  42. [42]

    B. G. Shin, J.-H. Park, J.-Y. Juo, J. Kong, and S. J. Jung, Structural-disorder-driven critical quantum fluc- tuation and localization in two-dimensional semiconduc- tors, Nature Communications14, 1 (2023)

  43. [43]

    A. D. Mirlin and Y. V. Fyodorov, Distribution of local densities of states, order parameter function, and critical behavior near the Anderson transition, Physical Review Letters72, 526 (1994)

  44. [44]

    Rodriguez, L

    A. Rodriguez, L. J. Vasquez, and R. A. R¨ omer, Multi- fractal Analysis with the Probability Density Function at the Three-Dimensional Anderson Transition, Physical Review Letters102, 106406 (2009)

  45. [45]

    Rodriguez, L

    A. Rodriguez, L. J. Vasquez, K. Slevin, and R. A. R¨ omer, Critical Parameters from a Generalized Multi- fractal Analysis at the Anderson Transition, Physical Re- view Letters105, 046403 (2010)

  46. [46]

    Rodriguez, L

    A. Rodriguez, L. J. Vasquez, K. Slevin, and R. A. R¨ omer, Multifractal finite-size scaling and universality at the An- derson transition, Physical Review B84, 134209 (2011). 9

  47. [47]

    Wess and B

    J. Wess and B. Zumino, Consequences of anomalous ward identities, Physics Letters B37, 95 (1971)

  48. [48]

    Witten, Global aspects of current algebra, Nuclear Physics B223, 422 (1983)

    E. Witten, Global aspects of current algebra, Nuclear Physics B223, 422 (1983)

  49. [49]

    Zhang, V

    Y. Zhang, V. W. Brar, F. Wang, C. Girit, Y. Yayon, M. Panlasigui, A. Zettl, and M. F. Crommie, Gi- ant phonon-induced conductance in scanning tunnelling spectroscopy of gate-tunable graphene, Nature Physics 4, 627 (2008)

  50. [50]

    Brihuega, P

    I. Brihuega, P. Mallet, C. Bena, S. Bose, C. Michaelis, L. Vitali, F. Varchon, L. Magaud, K. Kern, and J. Y. Veuillen, Quasiparticle Chirality in Epitaxial Graphene Probed at the Nanometer Scale, Physical Review Letters 101, 206802 (2008)

  51. [51]

    Rodriguez, L

    A. Rodriguez, L. J. Vasquez, K. Slevin, and R. A. R¨ omer, Multifractal finite-size scaling and universality at the An- derson transition, Physical Review B84, 134209 (2011)

  52. [52]

    V. Uski, R. A. R¨ omer, and M. Schreiber, Numerical study of eigenvector statistics for random banded ma- trices, Physical Review E65, 056204 (2002)

  53. [53]

    Terletska, Y

    H. Terletska, Y. Zhang, K.-M. Tam, T. Berlijn, L. Chion- cel, N. S. Vidhyadhiraja, and M. Jarrell, Systematic Quantum Cluster Typical Medium Method for the Study of Localization in Strongly Disordered Electronic Sys- tems, Applied Sciences8, 2401 (2018)

  54. [54]

    Schubert, J

    G. Schubert, J. Schleede, K. Byczuk, H. Fehske, and D. Vollhardt, Distribution of the local density of states as a criterion for Anderson localization: Numerically exact results for various lattices in two and three dimensions, Physical Review B81, 155106 (2010)

  55. [55]

    Asada, K

    Y. Asada, K. Slevin, and T. Ohtsuki, Anderson transi- tion in two-dimensional systems with spin-orbit coupling, Physical review letters89, 256601 (2002)

  56. [56]

    Eilmes and R

    A. Eilmes and R. A. R¨ omer, Exponents of the localiza- tion length in the 2d anderson model with off-diagonal disorder, physica status solidi (b)241, 2079 (2004)

  57. [57]

    Minakuchi, Two-dimensional random-network model with symplectic symmetry, Physical Review B58, 9627 (1998)

    K. Minakuchi, Two-dimensional random-network model with symplectic symmetry, Physical Review B58, 9627 (1998)

  58. [58]

    Schweitzer, Multifractal properties of critical eigen- states in two-dimensional systems with symplectic sym- metry, Journal of Physics: Condensed Matter7, L281 (1995)

    L. Schweitzer, Multifractal properties of critical eigen- states in two-dimensional systems with symplectic sym- metry, Journal of Physics: Condensed Matter7, L281 (1995)

  59. [59]

    Schweitzer and P

    L. Schweitzer and P. Markoˇ s, Disorder-driven splitting of the conductance peak at the Dirac point in graphene, Physical Review B78, 205419 (2008)

  60. [60]

    Potempa and L

    H. Potempa and L. Schweitzer, Localization of electrons in two-dimensional spatially-correlated random magnetic fields (1999)

  61. [61]

    Cuevas and V

    E. Cuevas and V. E. Kravtsov, Two-eigenfunction cor- relation in a multifractal metal and insulator, Physical Review B76, 235119 (2007)

  62. [62]

    Gade and F

    R. Gade and F. Wegner, The n= 0 replica limit of u (n) and u (n) so (n) models, Nuclear Physics B360, 213 (1991)

  63. [63]

    Gade, Anderson localization for sublattice models, Nuclear Physics B398, 499 (1993)

    R. Gade, Anderson localization for sublattice models, Nuclear Physics B398, 499 (1993)

  64. [64]

    Zhang, A

    H. Zhang, A. K. Grebenko, K. V. Iakoubovskii, H. Zhang, R. Yamaletdinov, A. Makarova, A. Fedorov, R. Sk, R. Shivajirao, Z. J. Tong, S. Grebenchuk, U. Karadeniz, L. Shi, D. V. Vyalikh, Y. He, A. Starkov, A. A. Alekseeva, C. C. Tee, C. M. Orofeo, J. Lin, K. Suenaga, M. Bosman, M. Koperski, B. Weber, K. S. Novoselov, O. V. Yazyev, C.-T. Toh, and B. ¨Ozyilmaz...