REVIEW 4 major objections 5 minor 55 references
The Hofstadter Butterfly: Bridging Condensed Matter, Topology, and Number Theory
T0 review · 4 major / 5 minor · reviewed 2026-08-06 · deepseek-v4-flash
Pith's one-line read The Hofstadter butterfly is generated by eight integer matrices acting on three integer labels, with gap Chern numbers as the integer slopes of its trapezoids.
desk verdict An elegant, heavily self-cited synthesis of prior results on the butterfly's number-theoretic structure; the eight-generator completeness claim is asserted, not proven, and the Mandelbrot analogy is a bonus rather than a result. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the eight-generator integer matrix scheme acting on the label vector $(q_R, q_L, \Delta\sigma)$. The six baby-butterfly generators are 3×3 unimodular matrices (Eq. 38) that combine the 2×2 flux recursions for $(q_R, q_L)$ with linear recursions for $\Delta\sigma$; the two tail generators $T_L$ and $T_R$ (Eq. 39) do the same for the chains. The central identity relating geometry to topology is that the Wannier-diagram trapezoid representing a butterfly has diagonals with integer slopes $\sigma_+$ and $-\sigma_-$, which are exactly the Chern numbers of the two X-shaped gaps, and these satisfy $\sigma_+ + \sigma_- = q_L + q_R$ and $q_L - q_R = N$. These integers are tied to the physics by the Diophantine gap-labeling equations $\sigma p + \tau q = r$ and $pN + qM = 1$. The mechanism does its work by turning the butterfly's self-similarity into matrix multiplication: repeated application of a generator, or of a product such as $T_L C_R$, gives a hierarchy whose scaling factor is an eigenvalue, a quadratic irrational of the form $[n^*+1; 1, n^*]$.
What would settle it
Compute the full set of integer labels $(q_R,q_L,\Delta\sigma)$ reachable from the parent $(1,1,0)$ by repeated application of the eight matrices, then compare it with the Wannier-diagram trapezoids obtained directly from Harper's equation for all rational flux $p/q$ with $q$ up to some bound; any unmatched trapezoid, or any generated trapezoid that does not correspond to a real gap, would disprove completeness.
Extended reading notes
Core claim
The paper claims that the Hofstadter butterfly is entirely generated by an eightfold prescription. Six matrices produce the six baby butterflies—upper and lower left and right, and central left and right—and two additional matrices produce the attached butterfly tails, which are infinite chains of shrinking butterflies. The matrices act on the integer triplet $(q_R, q_L, \Delta\sigma)$, where $q_R$ and $q_L$ are the denominators of the Farey-neighbour flux boundaries and $\Delta\sigma$ is the difference of the two gap Chern numbers; these three integers uniquely label each butterfly. In the geometric representation, each butterfly is a trapezoid whose diagonal slopes are the gap Chern numbers $(\sigma_+, -\sigma_-)$, with $\sigma_+ + \sigma_- = q_L + q_R$ and $q_L - q_R$ equal to the band Chern number $N$. Because every butterfly obeys the Farey sum rule, the recursions are simultaneously recursions of the Farey tree, and the same structure is mirrored in Möbius recursions of the Apollonian gasket and in the tree of primitive Pythagorean triples. The paper's claim is that the entire fractal, including self-similar hierarchies with scaling factors that are quadratic irrationals, follows from this integer matrix grammar.
Load-bearing premise
The eight matrices are presented as the complete generating prescription, but the recursion rules are extracted from inspecting the diagram and from earlier work rather than proved from Harper's equation; if any branch of the fractal is missed or mislabelled, the claimed completeness fails.
Editorial extensions
If this is right
- If the eight-generator scheme is complete, then the topological labels of every gap in the butterfly are determined recursively from the parent labels $(1,1,0)$, so no separate diagonalization is needed to know which Chern integers appear where.
- The E-cell and C-cell hierarchies have distinct scaling: for C-cells $\Delta\sigma$ stays constant while $q$ and $\sigma_\pm$ grow as powers of $\zeta$, whereas for E-cells $\Delta\sigma$ itself grows as $\zeta^l$; this gives a topological signature distinguishing the two families.
- Self-similar sub-butterflies are classified by an integer $n^*$ through the continued fraction $\zeta = [n^*+1; 1, n^*]$, but the same $n^*$ can label topologically distinct hierarchies, so the Chern numbers are required alongside $n^*$ for a complete label.
- The recasting of the butterfly recursions as Möbius transformations of Ford circles implies the fractal can be generated from Apollonian configurations, connecting the integer curvatures of the gasket to the integer slopes of the Wannier diagram.
- Observed Hofstadter spectra in moiré materials, such as magic-angle twisted bilayer graphene, should show the same integer-labeling pattern in their resolved gaps, providing a direct experimental fingerprint of the construction.
Reading between the lines
- A natural test of completeness beyond the paper's own checks is to generate all labels reachable from $(1,1,0)$ by the eight matrices up to a fixed generation and compare them one-to-one with Wannier-diagram trapezoids obtained numerically from Harper's equation; the paper does not present this exhaustive census.
- If the grammar is exact, then any physical perturbation that preserves the fractal's X-shaped gaps should also preserve the eight-matrix recursion for the Chern numbers, suggesting that the integer labels are robust quantized data even where the energy spectrum is deformed.
- The reappearance of the same eight matrices in the Apollonian and Pythagorean constructions suggests a stronger conjecture than the paper states: that the butterfly's self-similarity is isomorphic to the modular group action on rationals, so other $SL(2,\mathbb{Z})$-generated number-theoretic trees should also mirror butterfly sub-hierarchies.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents a largely expository account of the Hofstadter butterfly, arguing that the butterfly graph can be fully generated by eight unimodular matrices acting on integer labels (qR, qL, Δσ), with the gap Chern numbers appearing as integer slopes of trapezoid diagonals. The claimed structure is connected to the Farey tree, the Apollonian gasket, the Pythagorean tree, and the Mandelbrot set. The central constructive claim is that the eight 3×3 generators in Eqs. (38)-(39), together with the two tail generators, generate the entire butterfly hierarchy from the seed (1,1,0). The paper also contains a three-integer labeling theorem (§V.A), recursion relations for fluxes and Chern numbers (§VI), scaling exponents (§VII), and an Apollonian correspondence (§VIII). Much of the presentation is visual and pedagogical, with many figures illustrating the claimed identifications.
Significance. If the eight-generator completeness claim is correct, the paper offers a compact algebraic description of a well-studied quantum fractal and makes explicit a number-theoretic structure that has been developed piecemeal over the past decades. The explicit integer labeling and the connections to Farey tree, Apollonian gaskets, and Pythagorean triples are attractive and could be pedagogically useful. The paper is honest about its reliance on prior work, and the figures are informative. However, the central claim that these eight matrices generate the entire butterfly graph is asserted rather than proved, and several key identifications are stated without derivation or with apparent typographical errors. As a research contribution, the paper needs a rigorous completeness argument and correction of the Apollonian generator matrices before the central claim can be accepted.
major comments (4)
- [§VI.A and Eqs. (27)-(39)] The central claim that the eight generators (UL, UR, DL, DR, CL, CR, TL, TR) build the entire butterfly fractal is not proven. The recursions are said to follow from 'careful examination' and are attributed to refs. 11, 13, and 29, but no bijective or counting argument is given. The three-integer labeling theorem in §V.A is never turned into an exhaustive enumeration against which the eightfold prescription is checked. To support the 'entire butterfly fractal' claim, the authors should either prove by induction that every legal minimal-Δσ butterfly label (qR, qL, Δσ) appears on some orbit of the eight matrices, or provide an exhaustive enumeration for all Farey intervals up to a finite denominator bound and state the coverage result explicitly. Without this, the completeness of the eight-generator framework remains an assertion.
- [§VIII, Eqs. (51)-(53) and the matrices S1-S4] The four Apollonian generators S1, S2, S3, S4 are printed as identical 4×4 matrices in Section VIII. As written, these matrices cannot generate the Apollonian gasket, and the subsequent identifications in Section IX, such as h1 ≡ cL ↔ S1S2 and UL → S4S2, are therefore meaningless without the correct generator matrices. This is a concrete error in a section that is load-bearing for the butterfly-Apollonian bridge. Please provide the correct four matrices and verify that the products stated in Section IX reproduce the butterfly recursions.
- [§VI.C, Eqs. (40)-(43)] The reduction of the four E-cell generators UL, UR, DL, DR to a single E generator via the reparametrization (qs, qns, σs) is asserted rather than derived. In particular, the sharing rules in Eq. (42) and the definition α = σs − qns are stated without proof. Since this collapse is what preserves the distinction between UL and DL in the 3×3 matrix formulation, an incorrect sharing rule would erase the very information the larger matrices were introduced to keep. Please provide the explicit substitution of the matrices in Eq. (38) into the E-generator form of Eq. (43) and verify that the resulting action on (qR, qL, Δσ) reproduces exactly the four 3×3 matrices for several generations.
- [Appendix B, Eq. (B1)] The proof of the Farey sum rule in Appendix B rests on Eq. (B1), which is imported from refs. 11 and 28 without derivation or a statement of its precise domain of validity. Because Eq. (B1) is then used in Appendix B.1 to derive the butterfly recursions, any hidden assumption in B1 propagates into the rest of the paper. The status of B1 should be clarified: either present it as an assumption (with appropriate citation) or prove it within the appendix. As it stands, the Farey sum rule is not made self-contained, and the recursions derived from it inherit this limitation.
minor comments (5)
- [§V, Fig. 6 panel D and Eq. (22)] In the text describing Fig. 6, the y-coordinates of the upper corners are given as '1/qL and 1/qL'; the second should almost certainly be 1/qR. Additionally, Eq. (22) contains a mismatched bracket in the expression for σ− (the term 'qL]|' should be 'qL|'), and the quantities nL and nR are not defined before first use.
- [§II.B, Eq. (14)] In the transcription of the tight-binding eigenvalue equation, the term 'e2πiϕψ(y + a)' should presumably be 'e2πiϕψ(x, y + a)' or an equivalent expression; as written, the argument of ψ is incomplete.
- [§X, Butterfly meets Mandelbrot] The connection to the Mandelbrot set is presented as a suggestive analogy (mapping z to Eei2πϕ and matching Farey organization of bulbs and bands). As it stands, this is qualitative and does not amount to a mathematical correspondence. If this section is intended as a conjecture, that should be stated explicitly; otherwise, additional justification is needed.
- [Fig. 15 caption] The name 'Fransisco Claro' is a typo for 'Francisco Claro'.
- [General] Several passages repeat phrases almost verbatim (e.g., the 'derived through careful examination' sentence in §VI.A, and the introduction of Ford circles in §VIII, which is followed by a nearly identical restatement). A careful editorial pass would improve readability.
Circularity Check
The eight-generator butterfly construction is partly induced from the target graph and partly rests on the author's prior results, so the central completeness claim is partially circular.
-
fitted input called prediction
[Section VI (intro) and Section VI.A (Eqs. 27-39)]
"The butterfly graph is dissected into sextuplets of butterflies, labeled as (UL, UR, DL, DR, CL, CR). These labels denote six generators that are unimodular matrices with integer coefficients. Furthermore, each butterfly in the graph has an attached ”butterfly tail,” constructed using two additional generators, forming an eightfold prescription necessary to build the entire butterfly fractal. ... The ϕ recursions, derived through careful examination of the butterfly graph, are presented below."
The recursion rules are read directly off the butterfly graph ('careful examination') and then re-used as the generative engine claimed to 'build the entire butterfly fractal.' No counting or bijective argument shows that the eight matrices starting from (1,1,0) reach every legal butterfly and no more. In effect, the construction's output is the same pattern that was used as the input to define the generators, so the completeness claim is an assertion about the fitted rule rather than an independent derivation.
-
self citation load bearing
[Section V, after Eq. (23)]
"This corresponds to minimum value of ∆σ25, which is defined as: ∆σ = σ+ − σ−. ... Therefore, within a rectangular strip at flux values ( pL/qL, pR/qR), trapezoids with minimum violation of mirror symmetry form butterflies in the butterfly fractal25."
The identification of physical butterflies with minimum-Δσ trapezoids is imported from Ref. [25], a prior paper by the same author, and is not re-derived here. This rule is load-bearing: it decides which trapezoids are legal butterflies and hence which labels (qR,qL,Δσ) the eight matrices are supposed to generate. Without an independent proof that Harper gaps correspond exactly to this min-Δσ selection, the eight-generator completeness claim rests on an author-supplied premise rather than on the present derivation.
full rationale
The paper contains real mathematical content: the explicit 3x3 matrices in Eqs. (38)-(39), the derivation of the gap-Chern recursions from Eq. (19) and σ+ + σ− = qc, the Möbius construction of the Apollonian generators, and the mapping to Pythagorean triplets are not mere restatements. However, the central claim that these generators build the entire butterfly fractal is not derived from Harper's equation. The flux recursions are explicitly fitted to the graph ('careful examination'), and the min-Δσ selection rule is a same-author citation. Thus part of the derivation chain reduces to fitting or citing the target object it claims to generate. The score is 6 rather than 8 because independent derivations and explicit algebraic checks are present for substantial portions of the framework; the missing bijective completeness proof and the self-cited selection rule prevent the central claim from being fully self-contained.
Assumptions & free parameters
assumptions (8)
- domain assumption Harper equation describes the Hofstadter spectrum
- standard math Gap labeling theorem (Dana, Avron, Zak)
- domain assumption Chern numbers are topological integers given by TKNN
- domain assumption Farey sum rule holds for every butterfly
- ad hoc to paper The eight generator matrices (Eqs. 27-39) generate the complete butterfly hierarchy
- standard math Möbius transformations map Ford Apollonian configurations to each other
- standard math Pythagorean triple tree generates all primitive triples
- standard math Descartes' theorem for circle curvatures
Cite this review
Pith. "Pith review of The Hofstadter Butterfly: Bridging Condensed Matter, Topology, and Number Theory." pith.science (2026). https://pith.science/paper/EHFBNCOF
@misc{pith2026250713418,
author = {Pith},
title = {Pith review of: The Hofstadter Butterfly: Bridging Condensed Matter, Topology, and Number Theory},
year = {2026},
howpublished = {\url{https://pith.science/paper/EHFBNCOF}},
note = {Machine review of arXiv:2507.13418}
}
read the original abstract
Celebrating its golden jubilee, the Hofstadter butterfly fractal emerges as a remarkable fusion of art and science. This iconic X shaped fractal captivates physicists, mathematicians, and enthusiasts alike by elegantly illustrating the energy spectrum of electrons within a two dimensional crystal lattice influenced by a magnetic field. Enriched with integers of topological origin that serve as quanta of Hall conductivity, this quantum fractal and its variations have become paradigm models for topological insulators, novel states of matter in 21st century physics. This paper delves into the theoretical framework underlying butterfly fractality through the lenses of geometry and number theory. Within this poetic mathematics, we witness a rare form of quantum magic: Natures use of abstract fractals in crafting the butterfly graph itself. In its simplest form, the butterfly graph tessellates a two dimensional plane with trapezoids and triangles, where the quanta of Hall conductivity are embedded in the integer sloped diagonals of the trapezoids. The theoretical framework is succinctly expressed through unimodular matrices with integer coefficients, bringing to life abstract constructs such as the Farey tree, the Apollonian gaskets, and the Pythagorean triplet tree.
Figures
Figures from the paper (12 more)
Reference graph
Works this paper leans on
-
[1]
, Science 156, 636–638 (1967). B. B. Mandelbrot ``The Fractal Geometry of Nature
Mandelbrot, B. ``How long is the coast of Britain? Statistical self-similarity and fractional dimension", Science 156, 636–638 (1967). B. B. Mandelbrot ``The Fractal Geometry of Nature", (1982) (San Fransisco, CA: Freeman)
work page 1967
-
[2]
Hofstadter, Phys.Rev.B , 14 , (1976) 2239-49
D.R. Hofstadter, Phys.Rev.B , 14 , (1976) 2239-49
work page 1976
-
[3]
, G.H.Wannier, phys. stat. sol. (b) 88, 767 (1978)
`` ``A Result Not Dependent on Rationality for Bloch Electrons in a Magnetic Field", G.H.Wannier, phys. stat. sol. (b) 88, 767 (1978).",G. H. Wannier, Phys. Status Solidi B 88 , 757 (1978)
work page 1978
-
[4]
F. H. Claro and G.H. Wannier, Phys Rev B 19 (1979) 6068
work page 1979
- [5]
-
[6]
D.J. Thouless , M. Kohmoto , M. P. Nightingale and M. den Nijs, Phys. Rev. Lett. 49 ( 1982) 405
work page 1982
-
[7]
Developments in the quantum Hall effect
von Klitzing, Klaus (2005-09-15). "Developments in the quantum Hall effect". Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences. 363 (1834): 2203–2219
work page 2005
-
[8]
Kane C L and Mele E J 2006 Science 314 1692 Qi X-L and Zhang S-C 2010 Phys. Today January 33–8; I.I. Satija, The wonder of quantum spin , chapter 11 2 , Oxford University Press, 2024
work page 2006
Show all 55 references
-
[9]
I. I. Satija, Butterfly in the Quantum World IOP Concise, Morgan and Claypool, San Raffael, CA, 2016
2016
-
[10]
[11] I. I. Satija, Eur. Phys. J. - Special Topics, 225, 2533-47 (2016)
2016
-
[11]
Satija and M
I. Satija and M. Wilkinson, J. Phys A , 53 , 085703, 2020
2020
-
[12]
`` A Tisket, a Tasket, an Apollonian Gasket", Dana Mackenzie, American Scientist, 98 No 1 (2010)
2010
-
[13]
`` The interplay between topology and fractality of the Hofstadter butterfly", Indubala Satija, Physics Letter A Volume 552, 28 August 2025, 130635
2025
-
[14]
Phys, JETP 19 634, 1964
Mark Ya Azbel, Energy spectrum of a conduction electron in a magnetic field Sov. Phys, JETP 19 634, 1964
1964
-
[15]
Langbein D, `` The tight-binding and the nearly-free-electron approach to lattice electrons in external magnetic fields Phys
D. Langbein D, `` The tight-binding and the nearly-free-electron approach to lattice electrons in external magnetic fields Phys. Rev. 180 633, (1969)
1969
-
[16]
`` Cantor spectrum for the almost Mathieu operator", Commun. Math. Phys. 244 297; A Ávila A and S. Jitomirskaya S, The ten martini problem Ann. Math. 170 303 ( 2009)
2009
-
[17]
, Armelle Barelli, Jean Bellissard and Robert Fleckinger, ( unpublished ); ``Bloch electrons in a magnetic field
For review on this subject, see ``Bloch electrons on two-dimensional lattices in a magnetic field", Armelle Barelli, Jean Bellissard and Robert Fleckinger, ( unpublished ); ``Bloch electrons in a magnetic field" Hofstadter's butterfly" Ulrich R\" o ssler, Michael Suhrke (unpublished)
-
[18]
For a complete list of references, see `` Selected bibliography" in I. I. Satija, Butterfly in the Quantum World IOP Concise, Morgan and Claypool, San Raffael, CA, 2016
2016
-
[19]
Peierls R 1933 On the theory of diamagnetism of conduction electrons Z. Phys. 80 763–91; Roth L M 1962 Theory of bloch electrons in a magnetic field J. Phys. Chem. Solids 23 433
1933
-
[20]
Harper, Proc
P.G. Harper, Proc. Phys. Soc. A 68 ( 1955) 874
1955
-
[21]
& André, G
Aubry, S. & André, G. (1980). ``Analyticity Breaking and Anderson Localization in Incommensurate Lattices", Annals of the Israel Physical Society, 3, 133–164
1980
-
[22]
, J. Ketoja and I. Satija, 75 , (1995)
`` Self similarity and localization", J. Ketoja and I. Satija, 75 , (1995); "Harper Equation, Dissipative Standard Map and Strange Nonchaotic Attractors: Relationship between eigenvalue problem and Discrete Maps" Ketoja and Satija, Physica D 109D, 70 (1997). Ketoja and Satija;...
1995
-
[23]
RAY,Thesis, University of Oregon, 1978
R. RAY,Thesis, University of Oregon, 1978
1978
-
[24]
Danna, Y Avron and J
I. Danna, Y Avron and J. Zak, J. Phys C 18 L679 (1985); A. H. MacDonald , Phys. Rev. B 28 6713 (1983)
1985
-
[25]
I. I. Satija, Phys Rev E 104 044205 (2021)
2021
-
[26]
``The Quantum Phase Five Years After ",(Geometric Phases in Physics) ed A Shapere and F Wilczek (Singapore: World Scienti c) Michael Berry; 1988 Sci. Am. 46 December
1988
-
[27]
``Topology of Numbers by Allen Hatcher, ebook, published 2018
2018
-
[28]
[16] Schellnhuber H J, Obermair G M and Rauh A 1981 First-principles calculation of dimagnetic band-structure II: spectrum and wave-functions Phys. Rev. B 23 5191–202; Wilkinson M 1987 An exact effective Hamiltonian for a perturbed Landau level J. Phys. A: Math. Gen. 20 1761–71
1981
-
[29]
Wilkinson, J
M. Wilkinson, J. Phys. A: Math. Gen. 20 4337 ( 1987)
1987
-
[30]
Satija, J
I.I. Satija, J. Phys. A: Math. Theor. 54 ( 2020), 025701
2020
-
[31]
This proof is by Richard Friedberg ( private communication) July 2017
2017
-
[32]
Wilkinson, Proc
M. Wilkinson, Proc. Roy. Soc. A 391 305–50 (1984)
1984
-
[33]
Wilkinson J
M. Wilkinson J. Phys. A: Math, Gen.21 (1994) 8123-8148
1994
-
[34]
Simon, Adv
B. Simon, Adv. Appl. Math. 3 (1982) 463
1982
-
[35]
Jerzy Kocik, Proof of Descartes circle formula and its generalization, clarified (arXiv:0706.0372)
-
[36]
``Pythagorean Triplets, Integral Apollonians and The Hofstadter Butterfly", Indubala Satija, (2018) arXiv:1802.04585v3 [nlin.CD]
2018 arXiv
-
[37]
Berggren, ”Pytagoreiska triangular” (in Swedish), Elementa: Tidskrift fr elementŁr matematik, fysik och kemi 17 (1934), 129139.; ``Geneology of Pythagorean Triads" A
B. Berggren, ”Pytagoreiska triangular” (in Swedish), Elementa: Tidskrift fr elementŁr matematik, fysik och kemi 17 (1934), 129139.; ``Geneology of Pythagorean Triads" A. Hall, Math. Gazette 54, No. 390 (1970), 377-379
1934
-
[38]
Satija, arXiv:2104.13198v1 [math.GM]
``Kaleidoscopic Symmetries and Self-Similarity of Integral Apollonian Gaskets", I.I. Satija, arXiv:2104.13198v1 [math.GM]
-
[39]
L. R. Ford, The American Mathematical Monthly, Vol. 45, No. 9 ( 1938) 586-601
1938
-
[40]
Ogilvy, C. S. (1990). Excursions in Geometry. Dover. pp. 54 D 55. ISBN 0-486-26530-7
1990
-
[41]
Alperin, R.C. (2005). The modular tree of Pythagoras. American Mathematical Monthly, 112(9), 807–816; John Mack and Vic Czernezkyi, Australian Senior Mathematics Journal, 24 (2) 2010
2005
-
[42]
C. R. Dean, L. Wang, P. Maher, C. Forsythe, F. Ghahari, Y. Gao, J. Katoch, M. Ishigami, P. Moon, M. Koshino, T. Taniguchi, K. Watanabe, K. L. Shepard, J. Hone and P. Kim Nature 497 , 598–602 (2013)
2013
-
[43]
Nuckolls, Michael G
``Spectroscopy of the fractal Hofstadter energy spectrum", Kevin P. Nuckolls, Michael G. Scheer, Dillon Wong, Myungchul Oh, Ryan L. Lee, Jonah Herzog-Arbeitman, Kenji ,Watanabe3, Takashi Taniguchi4, Biao Lian & Ali Yazdani, 60 , Nature, 639, 2025
2025
-
[44]
MacDonald, Phys
``Theory of angle-resolved photoemission spectroscopy in graphene-based moiré superlattices" Jihang Zhu, Jingtian Shi , and Allan H. MacDonald, Phys. Rev. B 103, 235146 – Published 22 June, 2021
2021
-
[45]
Faddeev and R.M
``Generalized Bethe Ansatz Equations for Hofstadter Problem" L.D. Faddeev and R.M. Kashaev, commun. Math. Phys. 169 , 181 191 (1995)
1995
-
[46]
Peter Sarnak, ``Integral Apollonian Packings", The American Mathematical Monthly 118(4), March 2011
2011
-
[47]
ATHREYA, CRISTIAN COBELI, AND ALEXANDRU ZAHARESCU, International Mathematics Research Notices, Volume 2015, Issue 20, 2015, Pages 9991–10011
`` Radial density in Apollonian packings", JAYADEV S. ATHREYA, CRISTIAN COBELI, AND ALEXANDRU ZAHARESCU, International Mathematics Research Notices, Volume 2015, Issue 20, 2015, Pages 9991–10011
2015
-
[48]
1602.05111
Ávila A, Jitomirskaya S and Marx C A 2016 Spectral theory of extended Harper’s model and a question by Erdös and Szekeres, arxiv. 1602.05111
2016 arXiv
-
[49]
``Translational symmetry breaking and the disintegration of the Hofstadter butterfly", Archana Mishra, S. R. Hassan, R. Shankar, Phys. Rev. B 95, 035140 (2017)
2017
-
[50]
& Santos, L.H
``Unconventional self-similar Hofstadter superconductivity from repulsive interactions", Shaffer, D., Wang, J. & Santos, L.H. Unconventional self-similar Hofstadter superconductivity from repulsive interactions. Nat Commun 13, 7785 (2022).; ``Tuning the topology of p-wave supe...
2022
-
[51]
Satija and Erhai Zhao, Phys Rev B, 94 , 245128 (2016)
``Cosine edge modes in a periodically driven quantum system", Indubala I. Satija and Erhai Zhao, Phys Rev B, 94 , 245128 (2016)
2016
-
[52]
Anomalous edge states and topological phases of a kicked quantum Hall system
"Anomalous edge states and topological phases of a kicked quantum Hall system", Mahmoud Lababidi, Indubala I. Satija, Erhai Zhao, PRL Jan 15, 112 , 026805, 2014; ``Anatomy of a periodically driven p-wave superconductor", Erhai Zhao, arXiv:1603.08822 [cond-mat.supr-con]
2014 arXiv
-
[53]
Galitski, G
V. Galitski, G. Juzeliunas and I. B. Spielman, Phys. Today 72, 38 (2019)
2019
-
[54]
Linear-network model for magnetic breakdown in two dimensions
W.G Chambers, (1965), " Linear-network model for magnetic breakdown in two dimensions", Phys. Rev. A 140 A135 Gerlach E and Langbein D
1965
-
[55]
`` Field Theories of Condensed matter systems", Eduardo Fradkin, Addison-Wesley publishing company, 1991
1991
Reviewed August 6, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.