Bibliography and Paper Map
Reading guide for the generalized-symmetries course. This maps each reference to its role; it is not a complete bibliography of a field that would need several hundred entries. Every entry was verified against INSPIRE-HEP, arXiv or Crossref on 2026-09-27 (78 references; record in reviews/2026-09-27-comprehensive-review.md §6); new entries are verified when they are added.
How to read the references
Three levels, same discipline as the AQFT course:
The classic spine. Semester I primary material. These get read in full, and their central calculations get reproduced in problem sets. Most are short; the style is terse and the lecture notes supply the missing steps.
Books and reviews. Companions, not spines. Students keep two open per semester (Kogut + Savit in Sem I; McGreevy + Shao in Sem II) and consult the rest.
Research papers. Semester II seminar material. For each one, the presenter must identify: the technical claim, what it needs from Semester I, the one calculation worth reproducing, and the open problem it leaves.
The classic spine (Semester I)
| Reference | Course use | What to take from it |
|---|---|---|
| Kramers & Wannier, Phys. Rev. 60 (1941) 252 | Wk 4 | Order–disorder duality and T_c from self-duality; the oldest ancestor of every duality in the course. |
| Berezinskii, Sov. Phys. JETP 32 (1971) 493; Kosterlitz & Thouless, J. Phys. C 6 (1973) 1181 | Wks 1, 4 | Vortex unbinding; the energy–entropy argument in its original habitat. |
| Kadanoff & Ceva, Phys. Rev. B 3 (1971) 3918 | Wk 4 | Disorder variables μ and the order–disorder algebra; the seed of duality defects (Sem II Wk 13). |
| Wegner, J. Math. Phys. 12 (1971) 2259 | Wk 5 | ℤ₂ gauge theory; a phase transition with no local order parameter; Wilson loops before Wilson. |
| Wilson, Phys. Rev. D 10 (1974) 2445 | Wk 6 | Plaquette action, strong-coupling area law, confinement as a lattice statement. |
| Kogut & Susskind, Phys. Rev. D 11 (1975) 395 | Wk 7 | Hamiltonian lattice gauge theory; Gauss law; electric strings. |
| Villain, J. Physique 36 (1975) 581 | Wks 3, 9 | The periodic Gaussian action — the form in which every duality of the course is exact. |
| Elitzur, Phys. Rev. D 12 (1975) 3978 | Wk 5 | Local symmetries do not break; the theorem that forces loop diagnostics. |
| José, Kadanoff, Kirkpatrick, Nelson, Phys. Rev. B 16 (1977) 1217 | Wk 3; Sem II Wk 12 | The complete spin-wave ⊗ Coulomb-gas decomposition of the XY model. |
| Polyakov, Phys. Lett. B 59 (1975) 82; Nucl. Phys. B 120 (1977) 429 | Wks 9–10 | Monopole plasma, mass gap, permanent confinement in compact QED₃ — the semester’s central calculation. |
| Banks, Myerson, Kogut, Nucl. Phys. B 129 (1977) 493 | Wks 8, 11; Sem II Wk 12 | Exact duality of 4d Villain U(1); monopole Coulomb gas in 4d. |
| Guth, Phys. Rev. D 21 (1980) 2291 | Wk 11 (statement) | The Coulomb phase of 4d compact U(1) exists — the transition is real. |
| Nambu, Phys. Rev. D 10 (1974) 4262; Mandelstam, Phys. Rept. 23 (1976) 245 | Wk 11 | The dual-superconductor picture of confinement — see dual-superconductor. |
| ‘t Hooft, Nucl. Phys. B 138 (1978) 1 | Wks 11, 14 | Disorder loops, electric/magnetic flux classification; the operator language Sem II makes systematic. |
| Fradkin & Susskind, Phys. Rev. D 17 (1978) 2637 | Wks 4, 7 | Order and disorder in gauge systems; Hamiltonian dualities. |
| Fradkin & Shenker, Phys. Rev. D 19 (1979) 3682–3697 | Wks 13–14 | Gauge–Higgs phase diagrams; Higgs–confinement complementarity; what dynamical matter does to every diagnostic. |
| Cardy & Rabinovici, Nucl. Phys. B 205 (1982) 1 | Wk 12 | Oblique confinement and the SL(2,ℤ) structure of θ-vacua. |
| Creutz, Phys. Rev. D 21 (1980) 2308 | Wk 6 (mention) | Monte Carlo enters; where the analytic expansions hand off to the machine. |
Books and reviews (both semesters)
| Reference | Course use | Reading strategy |
|---|---|---|
| Kogut, Rev. Mod. Phys. 51 (1979) 659 | Sem I companion | The single best pedagogical source for Blocks A–C; read alongside every week. |
| Savit, Rev. Mod. Phys. 52 (1980) 453 | Sem I companion; Sem II Wk 14 §6 (finite abelian dualities) | Duality systematics; the tables of “theory ↔ dual theory” students should be able to re-derive. |
| Polyakov, Gauge Fields and Strings (1987), ch. 4 | Sem I Block C | The confinement chapters, in Polyakov’s own voice. |
| Fradkin, Field Theories of Condensed Matter Physics, 2nd ed. (2013) | Both semesters | The condensed-matter reading of gauge theories, disorder operators, and topological phases. |
| Tong, Lectures on Gauge Theory; Lectures on Statistical Field Theory | Sem I companion | When the originals are terse; the lattice and BKT chapters. |
| Wen, Quantum Field Theory of Many-Body Systems (2004) | Sem II Block 3 | Topological order from its inventor; string condensation. |
| Zeng, Chen, Zhou, Wen, Quantum Information Meets Quantum Matter (2019) | Sem II Blocks 3 | The quantum-information bridge, at textbook pace. |
| Preskill, Lecture Notes, ch. 9 | Sem II Blocks 3 | Topological quantum computation; the QEC reading of anyons. |
| Nakahara, Geometry, Topology and Physics, 2nd ed. | Sem I Wk 2 backup | Homology/cohomology chapters for students who want the continuum story. |
| McGreevy, arXiv:2204.03045 | Sem II companion | Generalized symmetries for condensed matter; the review to keep open all semester. |
| Shao, “What’s done cannot be undone” (TASI), arXiv:2308.00747 | Sem II companion | Non-invertible symmetries systematically; Blocks 4–5 follow its ordering. |
| Córdova, Dumitrescu, Intriligator, Shao (Snowmass), arXiv:2205.09545 | Sem II orientation | The field map; where each seminar paper sits. |
| Schäfer-Nameki, arXiv:2305.18296; Bhardwaj et al., arXiv:2307.07547; Brennan & Hong, arXiv:2306.00912 | Sem II alternates | Three more lecture-note routes through the same material; different students click with different ones. |
Generalized symmetries and anomalies (Semester II Blocks 1–2 spine)
| Reference | Course use | Required sections | Main technical input |
|---|---|---|---|
| Gaiotto, Kapustin, Seiberg, Willett, “Generalized global symmetries”, JHEP 02 (2015) 172, arXiv:1412.5148 | Block 1 target (Wk 1 seminar: §§2–3, §4.1, App. F; Wk 2: §§4.3, 5.2, App. B); Sem I Wks 14–15 | §§1–5, 7.2 + Maxwell/ℤ_N examples | p-form symmetries as topological operators; SSB of 1-form symmetries; gauging with backgrounds. |
| Kapustin & Seiberg, “Coupling a QFT to a TQFT and duality”, JHEP 04 (2014) 001, arXiv:1401.0740 | Block 1 support (Wk 2: §3) | §§1–3 | Coupling a QFT to a TQFT; what “sum over backgrounds” does to the operator spectrum. |
| Freed, Moore, Segal, “The uncertainty of fluxes”, Commun. Math. Phys. 271 (2007) 247 [hep-th/0605198]; “Heisenberg groups and noncommutative fluxes”, Ann. Phys. 322 (2007) 236 [hep-th/0605200] | Wk 1 (F7, Problem 8⋆⋆) | statements | Electric and magnetic fluxes do not commute: the Heisenberg group of a gauge theory on a spatial manifold. |
| Horowitz, “Exactly soluble diffeomorphism invariant theories”, Commun. Math. Phys. 125 (1989) 417 | Wk 2 | statements | BF theory as an exactly soluble topological field theory. |
| Maldacena, Moore, Seiberg, “D-brane charges in five-brane backgrounds”, JHEP 10 (2001) 005 [hep-th/0108152] | Wk 2 | the BF section | Level- BF theory and its finite Hilbert space on a torus. |
| Banks & Seiberg, “Symmetries and strings in field theory and gravity”, Phys. Rev. D 83 (2011) 084019 [1011.5120] | Wk 2 | §§2–4 | gauge theory as BF theory; discrete gauge symmetries and their charges. |
| Hofman & Iqbal, “Goldstone modes and photonization for higher form symmetries”, SciPost Phys. 6 (2019) 006 [arXiv:1802.09512] | Wk 3 | statements | The photon as the Goldstone boson of a spontaneously broken 1-form symmetry. |
| Lake, “Higher-form symmetries and spontaneous symmetry breaking”, arXiv:1802.07747 (preprint) | Wk 3 | statements | Goldstone theorem and Coleman–Mermin–Wagner bound for higher-form symmetries. |
| Tachikawa, “On gauging finite subgroups”, SciPost Phys. 8 (2020) 015 [arXiv:1712.09542] | Wk 4 | §§1–2 | Gauging a finite subgroup, the dual symmetry, and mixed anomalies. |
| Vafa, “Quantum symmetries of string vacua”, Mod. Phys. Lett. A 4 (1989) 1615 | Wk 4 (historical note) | statements | The quantum (dual) symmetry of an orbifold. |
| Aharony, Seiberg, Tachikawa, “Reading between the lines of four-dimensional gauge theories”, JHEP 08 (2013) 115 [arXiv:1305.0318] | Wk 4 (seminar: §§1.1–1.3, 2.1, 2.3, 6.4); Sem I Wk 14 | §§1–3 | Line-operator spectra of SU(N) vs SU(N)/ℤ_N; genuine vs non-genuine operators. |
| Gaiotto, Kapustin, Komargodski, Seiberg, “Theta, time reversal, and temperature”, JHEP 05 (2017) 091 [arXiv:1703.00501] | Block 2 target (Wk 5: App. D.1) | §§1–3 + one appendix calculation | The ℤ_N^(1) × T mixed anomaly at θ = π and its phase-diagram consequences. |
| ‘t Hooft, “Naturalness, chiral symmetry, and spontaneous chiral symmetry breaking”, NATO Sci. Ser. B 59 (1980) 135 (Cargèse 1979) | Wk 5 | the anomaly-matching argument | Anomaly matching with spectators. |
| Callan & Harvey, “Anomalies and fermion zero modes on strings and domain walls”, Nucl. Phys. B 250 (1985) 427 | Wk 5 | statements | Anomaly inflow from the bulk to defects. |
| Cheng & Seiberg, “Lieb–Schultz–Mattis, Luttinger, and ‘t Hooft — anomaly matching in lattice systems”, SciPost Phys. 15 (2023) 051 [arXiv:2211.12543] | Wk 5 | statements | LSM constraints as lattice anomalies. |
| Else & Nayak, “Classifying symmetry-protected topological phases through the anomalous action of the symmetry on the edge”, Phys. Rev. B 90 (2014) 235137 [arXiv:1409.5436] | Wks 5, 7 | statements | The edge action of the symmetry as the SPT invariant. |
| Ogata, Tachikawa, Tasaki, “General Lieb–Schultz–Mattis type theorems for quantum spin chains”, Commun. Math. Phys. 385 (2021) 79 [arXiv:2004.06458] | Wk 5 | statements | LSM theorems for chains with a projective symmetry per site. |
| Briegel & Raussendorf, “Persistent entanglement in arrays of interacting particles”, Phys. Rev. Lett. 86 (2001) 910 [quant-ph/0004051] | Wks 5, 7 | statements | The cluster state. |
| Majumdar & Ghosh, J. Math. Phys. 10 (1969) 1388 | Wk 5 (Problem) | statements | The Majumdar–Ghosh chain and its dimerized ground states. |
| ‘t Hooft, “A property of electric and magnetic flux in nonabelian gauge theories”, Nucl. Phys. B 153 (1979) 141 | Wk 6; Sem I Wk 14 | §§1–4 | Twisted boundary conditions on and the electric and magnetic flux sectors. |
| ‘t Hooft, “Some twisted selfdual solutions for the Yang–Mills equations on a hypertorus”, Commun. Math. Phys. 81 (1981) 267 | Wk 6 | statements | Constant-curvature self-dual solutions with fractional instanton number. |
| Witten, “Large N chiral dynamics”, Ann. Phys. 128 (1980) 363 | Wk 6 | statements | θ-dependence at large N and the multibranch vacuum energy. |
| Witten, “Theta dependence in the large N limit of four-dimensional gauge theories”, Phys. Rev. Lett. 81 (1998) 2862 [hep-th/9807109] | Wk 6 | statements | The branch structure of the vacuum energy at large N. |
| Lüscher, “Topology of lattice gauge fields”, Commun. Math. Phys. 85 (1982) 39 | Wk 6 | statements | The topological charge of lattice gauge fields. |
| Chen, Gu, Liu, Wen, “Symmetry protected topological orders and the group cohomology of their symmetry group”, Phys. Rev. B 87 (2013) 155114 [arXiv:1106.4772] | Wk 7 | 1d classification + statements | SPT classification by group cohomology. |
| Affleck, Kennedy, Lieb, Tasaki, Phys. Rev. Lett. 59 (1987) 799 | Wk 7 | statements | The AKLT chain: a valence-bond solid with spin-½ edges. |
| Haldane, Phys. Lett. A 93 (1983) 464; Phys. Rev. Lett. 50 (1983) 1153 | Wk 7 | statements | The Haldane gap of integer-spin chains. |
| den Nijs & Rommelse, Phys. Rev. B 40 (1989) 4709 | Wk 7 | statements | String order in the Haldane phase. |
| Pérez-García, Wolf, Sanz, Verstraete, Cirac, Phys. Rev. Lett. 100 (2008) 167202 [0802.0447] | Wk 7 | statements | String order and symmetries in MPS: the virtual action of a symmetry. |
| Pollmann, Turner, Berg, Oshikawa, Phys. Rev. B 81 (2010) 064439 [0910.1811] | Wk 7 | statements | Entanglement spectrum and the protection of the Haldane phase. |
| Chen, Gu, Wen, “Classification of gapped symmetric phases in one-dimensional spin systems”, Phys. Rev. B 83 (2011) 035107 [1008.3745] | Wk 7 | statements | The MPS classification of 1d SPT phases by . |
| Levin & Gu, Phys. Rev. B 86 (2012) 115109 [1202.3120] | Wk 7 seminar (§§I–III, V.A) | §§I–III, V.A | Braiding statistics approach to SPT phases; gauging the SPT. |
| Raussendorf & Briegel, Phys. Rev. Lett. 86 (2001) 5188 | Wk 7 | statements | The cluster state as a resource. |
| Else, Schwarz, Bartlett, Doherty, Phys. Rev. Lett. 108 (2012) 240505 [1201.4877] | Wk 7 | statements | SPT order and measurement-based computation. |
| Vishwanath & Senthil, Phys. Rev. X 3 (2013) 011016 [1209.3058] | Wk 7 | statements | Bosonic SPT phases beyond group cohomology in 3+1d. |
| Dijkgraaf & Witten, Commun. Math. Phys. 129 (1990) 393 | Wk 7 | §6 (finite groups) | Topological gauge theories from group cocycles; the toric-code/double-semion dichotomy. |
| Lieb, Schultz, Mattis, Ann. Phys. 16 (1961) 407; Oshikawa, Phys. Rev. Lett. 84 (2000) 1535; Hastings, Phys. Rev. B 69 (2004) 104431 [cond-mat/0305505] | Wk 5 | statements + flux-threading argument | LSM as a lattice anomaly; the theorem that makes anomalies concrete for spin chains. |
Topological order and quantum information (Semester II Block 3 spine)
| Reference | Course use | Required sections | Main technical input |
|---|---|---|---|
| Kitaev, “Fault-tolerant quantum computation by anyons”, Ann. Phys. 303 (2003) 2 [quant-ph/9707021] | Wk 2 seminar; Wk 8 target; Wk 10 | the sections on toric codes, abelian anyons and materialized symmetry (§§1–3 of the arXiv text) | The toric code: stabilizers, anyons, fault tolerance. |
| Kitaev, “Anyons in an exactly solved model and beyond”, Ann. Phys. 321 (2006) 2 [cond-mat/0506438] | Wk 7 (App. E, anyon data); Wk 8 (App. E.4–E.5); Wk 10; Wk 11 (§§8.3–8.6, §9, App. E.1–E.2) | §§1–2 skim | The honeycomb model; anyon theory in its mature form (appendix as reference, not reading). |
| Kitaev & Preskill, Phys. Rev. Lett. 96 (2006) 110404 [hep-th/0510092]; Levin & Wen, Phys. Rev. Lett. 96 (2006) 110405 [cond-mat/0510613] | Wk 9 | full (both are 4 pages) | Topological entanglement entropy, two constructions. |
| Kirillov & Balsam, “Turaev–Viro invariants as an extended TQFT”, arXiv:1004.1533 | Wk 11 | statements | The Levin–Wen models as Turaev–Viro state sums; the doubled content of a string net. |
| Laughlin, Phys. Rev. Lett. 50 (1983) 1395 | Wk 10 | statements | The ν = 1/3 state. |
| Arovas, Schrieffer, Wilczek, Phys. Rev. Lett. 53 (1984) 722 | Wk 10 | statements | Fractional statistics of the Laughlin quasiholes. |
| Wen, Phys. Rev. B 41 (1990) 12838 | Wk 10 | statements | Chiral edge states of fractional quantum Hall states. |
| Wen & Zee, Phys. Rev. B 46 (1992) 2290 | Wk 10 | statements | The K-matrix classification of abelian quantum Hall states. |
| Witten, “The Chern–Simons function and the quantum Hall effect”, to appear in Bull. Amer. Math. Soc. [arXiv:2609.21182] | Sem I Wk 12; Sem II Wk 10 | §§1–4 | The θ-term and the Chern–Simons function from a 4-manifold extension, integrality on spin manifolds, the integer Hall level and the emergent-field model of the fractional effect. |
| Witten, “Quantum field theory and the Jones polynomial”, Commun. Math. Phys. 121 (1989) 351 | Wk 10 | statements | Chern–Simons theory, Wilson lines and their framing. |
| Coste, Gannon, Ruelle, Nucl. Phys. B 581 (2000) 679 [hep-th/0001158] | Wk 10 | statements | The modular data of finite-group quantum doubles. |
| Levin & Wen, “Fermions, strings, and gauge fields in lattice spin models”, Phys. Rev. B 67 (2003) 245316 [cond-mat/0302460] | Wk 8 | statements | Anyon statistics from string operators: the T-junction argument. |
| Bais & Slingerland, “Condensate induced transitions between topologically ordered phases”, Phys. Rev. B 79 (2009) 045316 [arXiv:0808.0627] | Wk 8 | statements | Rules for anyon condensation. |
| Castelnovo & Chamon, “Quantum topological phase transition at the microscopic level”, Phys. Rev. B 77 (2008) 054433 [arXiv:0707.2084] | Wk 11 | statements | A deformed toric-code wave function whose topological entropy vanishes beyond a transition. |
| Hamma, Ionicioiu, Zanardi, Phys. Rev. A 71 (2005) 022315 [quant-ph/0409073] | Wk 9 | statements | The bipartite entanglement of the toric code from its stabilizer group. |
| Bravyi & Kitaev, “Quantum codes on a lattice with boundary”, quant-ph/9811052 | Wk 9 | statements | The planar code with rough and smooth boundaries. |
| Bravyi, Hastings, Verstraete, Phys. Rev. Lett. 97 (2006) 050401 [quant-ph/0603121] | Wk 9 | statements | Lieb–Robinson bounds and the generation of topological order. |
| Bravyi, Hastings, Michalakis, J. Math. Phys. 51 (2010) 093512 [1001.0344] | Wk 9 | statements | Stability of topological order under local perturbations. |
| Honecker, Picco, Pujol, Phys. Rev. Lett. 87 (2001) 047201 [cond-mat/0010143] | Wk 9 | the value | The Nishimori point of the 2d random-bond Ising model. |
| Wang, Harrington, Preskill, Ann. Phys. 303 (2003) 31 [quant-ph/0207088] | Wk 9 | the thresholds 0.0293(2) and 0.1031(1) | Toric-code thresholds with and without measurement errors. |
| Zou & Haah, Phys. Rev. B 94 (2016) 075151 [1604.06101] | Wk 9 | statements | Spurious topological entanglement entropy. |
| Levin & Wen, “String-net condensation: a physical mechanism for topological phases”, Phys. Rev. B 71 (2005) 045110 [cond-mat/0404617] | Wk 11 target | §§1–4 + ℤ₂ example | String-net condensation; F-symbols; emergent gauge theory. |
| Wen, Int. J. Mod. Phys. B 4 (1990) 239; Wen & Niu, Phys. Rev. B 41 (1990) 9377 | Wk 2 (optional), Wk 8 context, Wk 10 seminar | statements | Topological order named and defined; GSD on higher genus. |
| Chen, Gu, Wen, Phys. Rev. B 82 (2010) 155138 [arXiv:1004.3835] | Wk 9 | §§II–V | Phases as local-unitary equivalence classes; long-range entanglement. |
| Dennis, Kitaev, Landahl, Preskill, J. Math. Phys. 43 (2002) 4452 [quant-ph/0110143] | Wk 9 | §§I, III.A–B, IV | The toric code as a quantum memory; error models and thresholds. |
| Hansson, Oganesyan, Sondhi, “Superconductors are topologically ordered”, Ann. Phys. 313 (2004) 497 [cond-mat/0404327] | Wks 2, 3 (seminar); Sem I Wk 14 | §§I–IV, V.A–B (Roman numbering) | Superconductors are topologically ordered; the 1-form-symmetry reading of BCS. |
| Trebst, Werner, Troyer, Shtengel, Nayak, “Breakdown of a topological phase: quantum phase transition in a loop gas model with tension”, Phys. Rev. Lett. 98 (2007) 070602 [cond-mat/0609048]; Tupitsyn, Kitaev, Prokof’ev, Stamp, “Topological multicritical point in the toric code and 3D gauge Higgs models”, Phys. Rev. B 82 (2010) 085114 [arXiv:0804.3175] | Wk 8 + write-up topic 2; Sem I Wks 13–14 | phase diagrams | The perturbed toric code = the Fradkin–Shenker diagram, numerically mapped. |
The modern lattice synthesis and condensation defects (Semester II Blocks 4–5 spine)
| Reference | Course use | Required sections | Main technical input |
|---|---|---|---|
| Sulejmanpasic & Gattringer, “Abelian gauge theories on the lattice: θ-terms and compact gauge theory with(out) monopoles”, Nucl. Phys. B 943 (2019) 114616 [arXiv:1901.02637] | Wk 12; Sem I Wk 12 | §§1–3 | Monopole-free compact lattice QED; well-defined lattice θ-terms. |
| Gorantla, Lam, Seiberg, Shao, “A modified Villain formulation of fractons and other exotic theories”, J. Math. Phys. 62 (2021) 102301 [arXiv:2103.01257] | Wk 2 (App. C.2, the BF dictionary); Wk 12 target (§1.2, Apps. B.1, C.1) | Villain sections (skip fracton applications on first pass) | The modified Villain systematics: exact dualities, exact higher-form symmetries, exact anomalies on the lattice. |
| Chen & Tata, “Higher cup products on hypercubic lattices: application to lattice models of topological phases”, J. Math. Phys. 64 (2023) 091902 [arXiv:2106.05274] | Wks 6, 12 reference | as needed | Higher cup products on hypercubic lattices; the sign conventions conventions adopts. |
| Koide, Nagoya, Yamaguchi, PTEP 2022 (2022) 013B03 [2109.05992] | Wk 13 (statement); Wk 14 (optional) | abstract | Non-invertible topological defects in 4d gauge theory. |
| Fröhlich, Fuchs, Runkel, Schweigert, Phys. Rev. Lett. 93 (2004) 070601 [cond-mat/0404051] | Wk 13 (history) | statements | Kramers–Wannier duality from conformal defects. |
| Seiberg & Shao, SciPost Phys. 16 (2024) 064 [2307.02534] | Wk 13 | statements | Majorana chain and Ising model: non-invertible translations, anomalies and emanant symmetries. |
| Aasen, Mong, Fendley, “Topological defects on the lattice I: the Ising model”, J. Phys. A 49 (2016) 354001 [arXiv:1601.07185] | Wk 13 target | §§1–4 | The Kramers–Wannier duality defect on the lattice Ising model. |
| Burnell, “Anyon condensation and its applications”, Ann. Rev. Condens. Matter Phys. 9 (2018) 307 [arXiv:1706.04940] | Wk 15 (reading list, open problem 10 of Wk 14) | statements | Anyon condensation beyond the abelian case. |
| Nandkishore & Hermele, “Fractons”, Ann. Rev. Condens. Matter Phys. 10 (2019) 295 [arXiv:1803.11196] | Wk 15 (reading list, open problem 9 of Wk 14) | statements | Fracton phases. |
| Seiberg & Shao, “Exotic ℤ_N symmetries, duality, and fractons in 3+1-dimensional quantum field theory”, SciPost Phys. 10 (2021) 003 [arXiv:2004.06115] | Wk 15 (reading list, open problem 9 of Wk 14) | statements | Exotic subsystem symmetries and their lattice models. |
| Tantivasadakarn, Thorngren, Vishwanath, Verresen, “Long-range entanglement from measuring symmetry-protected topological phases”, Phys. Rev. X 14 (2024) 021040 [arXiv:2112.01519] | Wk 15 (reading list, open problem 11 of Wk 14) | statements | Gauging by measurement. |
| Guimaraes, “Finite-cost currents at higher-gauging walls in four-dimensional ℤ_N gauge theory”, manuscript in preparation (version 25, 2026-09-20; not submitted) | Wk 14 target + master-project | §§1–9 and the appendices | The group’s manuscript: the higher-gauging wall, its endpoint currents, the clock dual and the endpoint tension. |
| Choi, Córdova, Hsin, Lam, Shao, “Non-invertible condensation, duality, and triality defects in 3+1 dimensions”, Commun. Math. Phys. 402 (2023) 489 [arXiv:2204.09025] | Wk 14 | statements | Condensation defects in 3+1d. |
| Bah, Leung, Waddleton, “On the physics of higher condensation defects”, JHEP 09 (2026) 272 [arXiv:2506.04346] | Wk 14 | statements | The four-dimensional subgroup condensation defect with its worldvolume symmetries and fusion data; the construction the manuscript names as closest to its wall. |
| Córdova, Costa, Hsin, “Non-invertible symmetries as condensation defects in finite-group gauge theories”, arXiv:2412.16681 | Wk 14 (optional) | statements | Lattice gauging interfaces. |
| Hofmeier, Pimenta, Cao, “Lattice gauging interfaces and noninvertible defects in higher dimensions”, arXiv:2605.12601 | Wk 14 (optional) | statements | Lattice gauging interfaces. |
| Xue, Yang, Zhang, “On gauging finite symmetries by higher gauging condensation defects”, JHEP 08 (2026) 179 [arXiv:2512.22440] | Wk 14 (optional) | statements | Gauging by condensation defects. |
| Choi, Sanghavi, Shao, Zheng, “Non-invertible and higher-form symmetries in 2+1d lattice gauge theories”, SciPost Phys. 18 (2025) 008 [arXiv:2405.13105] | Wk 14 (optional) | statements | Lattice duality defects in 2+1d gauge theories. |
| Ukawa, Windey, Guth, “Dual variables for lattice gauge theories and the phase structure of Z(N) systems”, Phys. Rev. D 21 (1980) 1013; Nguyen, Sulejmanpasic, Ünsal, Phys. Rev. Lett. 134 (2025) 141902 [arXiv:2401.04800] | Wk 14 (optional) | statements | The phase structure of ℤ_N gauge theories. |
| Janke & Villanova, Nucl. Phys. B 489 (1997) 679 [hep-lat/9612008]; Karsch & Stickan, Phys. Lett. B 488 (2000) 319 [hep-lat/0007019]; Xu, Sun, Lv et al., Phys. Rev. B 100 (2019) 064525 [1908.10990]; Ditzian et al., Phys. Rev. B 22 (1980) 2542 and Todoroki et al. [cond-mat/0207665] (these two as the manuscript cites them, not checked on INSPIRE) | Wk 14 (optional) | critical couplings | Three-dimensional clock and Potts models. |
| Grigorio, Guimaraes, Oliveira et al., “U(1) effective confinement theory from SU(2) restricted gauge theory via the Julia–Toulouse approach”, Phys. Lett. B 697 (2011) 392 [arXiv:1010.6215] | Wk 14 | statements | The group’s Julia–Toulouse treatment of restricted SU(2), as the manuscript cites it. |
| Roumpedakis, Seifnashri, Shao, “Higher gauging and non-invertible condensation defects”, Commun. Math. Phys. 401 (2023) 3043 [arXiv:2204.02407] | Wk 13–14 target | §§1–3 + condensation-defect construction | Higher gauging; condensation defects; projector fusion — the framework the manuscript takes as prior work. |
| Choi, Córdova, Hsin, Lam, Shao, Phys. Rev. D 105 (2022) 125016 [arXiv:2111.01139]; Kaidi, Ohmori, Zheng, Phys. Rev. Lett. 128 (2022) 111601 [arXiv:2111.01141] | Wks 12–13 (statement) | intros | Non-invertible duality defects in 3+1d from half-space gauging. |
| Julia & Toulouse, J. Physique Lett. 40 (1979) L-395 | Sem I Wk 11; Wk 14 | full (it is 4 pages) | The original: defect condensation changes the effective field content. |
| Quevedo & Trugenberger, Nucl. Phys. B 501 (1997) 143 [hep-th/9604196] | Sem I Wk 11; Wk 14 | §§1–3 | The JTA in field-theory form; rank-changing condensation — see julia-toulouse-mechanism. |
| The group’s JTA series: Grigorio, Guimaraes, Wotzasek, Phys. Lett. B 674 (2009) 213 [0808.3698] (monopoles with a Chern–Simons term); Grigorio, Guimaraes, Rougemont, Wotzasek, Phys. Lett. B 690 (2010) 316 [0908.0370] (dual approaches to defect condensation); Grigorio, Guimaraes, Rougemont, Wotzasek, JHEP 08 (2011) 118 [1102.3933] (confinement and brane symmetry); Grigorio, Guimaraes, Rougemont, Wotzasek, Zarro, Phys. Rev. D 86 (2012) 027705 [1202.3798] (the BF theory as an electric JT condensate); Guimaraes, Rougemont, Wotzasek, Zarro, Phys. Rev. D 86 (2012) 125039 [1209.2751] (the bosonized Schwinger model); Guimaraes, Rougemont, Wotzasek, Zarro, Phys. Lett. B 723 (2013) 422 [1209.3073] (electric condensate and magnetic confinement); Grigorio, Guimaraes, Rougemont, Wotzasek, Zarro, Phys. Rev. D 88 (2013) 065009 [1307.1035] (Chern–Simons term in a dual Josephson junction) | Wks 9, 11, 14 | selected | The confinement-duality line this course descends from. Cite papers individually: “PRD 86” alone is ambiguous. In the BF language, level-one with the original photon is the electric condensate (PRD 86 027705, PLB 723); the magnetic condensate is the massive Kalb–Ramond form, dual to . |
Block A additions (2026-07-07 notes rewrite)
References introduced by the full Semester I Block A lecture notes, per the citation gate of the note-quality-template.
| Reference | Used in | What for |
|---|---|---|
| Kosterlitz, J. Phys. C 7 (1974) 1046 | Wk 4 | the RG flow equations |
| Nelson & Kosterlitz, Phys. Rev. Lett. 39 (1977) 1201 | Wks 1, 4 | the universal stiffness jump |
| Bishop & Reppy, Phys. Rev. Lett. 40 (1978) 1727 | Wks 1, 4 | torsional-oscillator measurement of the jump |
| Kardar, Statistical Physics of Fields, CUP 2007, ch. 8 (the sections on topological defects in the XY model and on the renormalization group of the Coulomb gas) | Wk 4 | RG derivation in matching conventions |
| Minnhagen, Rev. Mod. Phys. 59 (1987) 1001 | Wk 4 | Coulomb-gas review; first-order caveat at large fugacity |
| Fröhlich & Spencer, Comm. Math. Phys. 81 (1981) 527 | Wk 3 | rigorous existence of the BKT transition via the Coulomb gas |
| Mermin & Wagner, Phys. Rev. Lett. 17 (1966) 1133; Hohenberg, Phys. Rev. 158 (1967) 383 | Wk 1 | no continuous-symmetry breaking in |
| Spitzer, Principles of Random Walk, 2nd ed., Springer 1976, §15 | Wk 1 | lattice Green function asymptotics (the constant κ) |
| Onsager, Phys. Rev. 65 (1944) 117 | Wk 4 | exact Ising solution (context for Kramers–Wannier) |
| Peierls, Proc. Camb. Phil. Soc. 32 (1936) 477 | Wk 4 | existence of the Ising transition (duality only locates it) |
| Chui & Weeks, Phys. Rev. B 14 (1976) 4978 | Wk 3 | roughening ↔ BKT correspondence for the height model |
| Chaikin & Lubensky, Principles of Condensed Matter Physics, CUP 1995, §9 | Wk 1 | vortices and stiffness in laboratory language |
Additions from the 2026-09-27 review
References that the Semester I notes use or quote but that were missing here, all verified against INSPIRE on 2026-09-27.
| Reference | Used in | What for |
|---|---|---|
| Hasenbusch, J. Phys. A 38 (2005) 5869 [cond-mat/0502556] | Wks 1, 3, 4 | bare critical coupling of the cosine XY model, |
| Janke & Nather, Phys. Rev. B 48 (1993) 7419 | Wks 1, 3, 4 | bare critical coupling of the Villain XY model, |
| Kogut, “The lattice gauge theory approach to quantum chromodynamics” (printed title; INSPIRE lists “A review of the lattice gauge theory approach…”), Rev. Mod. Phys. 55 (1983) 775 | Wks 6, 7 | strong-coupling methods and roughening (§§IV.A, V.A, V.C) |
| ‘t Hooft, “Gauge fields with unified weak, electromagnetic, and strong interactions”, EPS International Conference on High-Energy Physics, Palermo, 23–28 June 1975, p. 1225 | Wk 11 | the dual-superconductor proposal |
| Witten, Phys. Lett. B 86 (1979) 283 | Wk 12 | the Witten effect |
| Wilczek, Phys. Rev. Lett. 58 (1987) 1799 | Wk 12 | axion electrodynamics |
| Osterwalder & Seiler, “Gauge field theories on the lattice”, Ann. Phys. 110 (1978) 440 | Wks 10, 13 | the convergent expansion behind Higgs–confinement complementarity |
| Svetitsky & Yaffe, Nucl. Phys. B 210 (1982) 423 | Wks 10, 14 | universality of the deconfinement transition |
| Göpfert & Mack, Commun. Math. Phys. 82 (1982) 545 (the volume spans 1981–82; INSPIRE lists 1981, the journal header 1982; Villain action, Theorem 1, Corollary 2, eq. (1.8a) for the Debye mass) | Wks 9–10 | confinement of static charges in 3d lattice gauge theory at all couplings |
| Fröhlich & Spencer, Commun. Math. Phys. 83 (1982) 411 | Wk 11 | the massless (Coulomb) phase of 4d abelian lattice gauge theory |
| Arnold, Bunk, Lippert, Schilling, “Compact QED under scrutiny: it’s first order”, Nucl. Phys. B Proc. Suppl. 119 (2003) 864 [hep-lat/0210010] | Wk 11 | the order of the 4d Wilson-action transition, |
| ‘t Hooft, “Topology of the gauge condition and new confinement phases in nonabelian gauge theories”, Nucl. Phys. B 190 (1981) 455 | Wk 11 | abelian projection |
| Seiberg & Witten, “Electric–magnetic duality, monopole condensation, and confinement in N=2 supersymmetric Yang–Mills theory”, Nucl. Phys. B 426 (1994) 19; Erratum 430 (1994) 485 [hep-th/9407087] | Wk 11 | a controlled realization of monopole condensation |
| Cardy, “Duality and the θ parameter in abelian lattice models”, Nucl. Phys. B 205 (1982) 17 | Wk 12 | oblique confinement on the lattice |
| Witten, “On S-duality in abelian gauge theory”, Selecta Math. 1 (1995) 383 [hep-th/9505186] | Wk 12 | the SL(2,ℤ) action on abelian gauge theory |
| Qi, Hughes, Zhang, “Topological field theory of time-reversal invariant insulators”, Phys. Rev. B 78 (2008) 195424 [0802.3537] | Wk 12 | θ = π in topological insulators |
| Zyuzin & Burkov, “Topological response in Weyl semimetals and the chiral anomaly”, Phys. Rev. B 86 (2012) 115133 [1206.1868] | Wk 12 | the axion response of Weyl semimetals |
| Vazifeh & Franz, “Electromagnetic response of Weyl semimetals”, Phys. Rev. Lett. 111 (2013) 027201 [1303.5784] | Wk 12 | absence of the chiral magnetic effect in equilibrium |
| Braga, Guimaraes, Paganelly, “Multivalued fields and monopole operators in topological superconductors”, Ann. Phys. 419 (2020) 168245 [1812.01705]; Chrispim, Bruni, Guimaraes, “Massive photon propagator in the presence of axionic fluctuations”, Phys. Rev. B 103 (2021) 165120 [2012.00184] | Wk 12 | the group’s condensed-matter line |
| Fredenhagen & Marcu, “Charged states in ℤ₂ gauge theories”, Commun. Math. Phys. 92 (1983) 81; “A confinement criterion for QCD with dynamical quarks”, Phys. Rev. Lett. 56 (1986) 223 | Wk 13 | the Fredenhagen–Marcu order parameter |
| Fröhlich, Morchio, Strocchi, “Higgs phenomenon without symmetry breaking order parameter”, Nucl. Phys. B 190 (1981) 553 | Wk 13 | gauge-invariant description of the Higgs phase |
| Jongeward, Stack, Jayaprakash, Phys. Rev. D 21 (1980) 3360 | Wk 13 | Monte Carlo phase diagram of the ℤ₂ gauge–Higgs model |
| Griffiths, J. Math. Phys. 8 (1967) 478; Ginibre, Commun. Math. Phys. 16 (1970) 310 | Wk 13 | correlation inequalities behind |
| Kotecký & Preiss, Commun. Math. Phys. 103 (1986) 491 | Wk 13 | the convergence criterion of the polymer expansion |
| Somoza, Serna, Nahum, “Self-dual criticality in three-dimensional ℤ₂ gauge theory with matter”, Phys. Rev. X 11 (2021) 041008 [2012.15845] | Wk 13 | the multicritical point on the self-dual line |
| Kajantie, Laine, Rummukainen, Shaposhnikov, Phys. Rev. Lett. 77 (1996) 2887 [hep-ph/9605288]; Rummukainen, Tsypin, Kajantie, Nucl. Phys. B 532 (1998) 283 [hep-lat/9805013] | Wk 13 | the endpoint of a Higgs first-order line and its Ising class |
| Polyakov, “Thermal properties of gauge fields and quark liberation”, Phys. Lett. B 72 (1978) 477; Susskind, “Lattice models of quark confinement at high temperature”, Phys. Rev. D 20 (1979) 2610 | Wk 14 | the Polyakov loop as the order parameter of deconfinement |
| Greensite, An Introduction to the Confinement Problem, Lecture Notes in Physics 821, Springer 2011 (book, not checked) | Wk 14 | center symmetry and confinement criteria |
| Blöte & Deng, “Cluster Monte Carlo simulation of the transverse Ising model”, Phys. Rev. E 66 (2002) 066110 | Wk 7 | the critical point of the d gauge theory through its dual transverse-field Ising model |
| NIST Digital Library of Mathematical Functions, §28.8 (Mathieu functions, asymptotics for large q), https://dlmf.nist.gov/28.8 | Wk 7 | the one-plaquette tunnelling splitting |
| Drouffe & Itzykson, “Lattice gauge fields”, Phys. Rep. 38 (1978) 133 | Wk 6 | strong-coupling and character-expansion methods |
| Ferrenberg, Xu, Landau, “Pushing the limits of Monte Carlo simulations for the 3d Ising model”, Phys. Rev. E 97 (2018) 043301 [arXiv:1806.03558] | Wks 5, 14 | the 3d Ising critical coupling , hence of 3d gauge theory |
| Amit, Goldschmidt, Grinstein, “Renormalization group analysis of the phase transition in the 2D Coulomb gas, sine-Gordon theory and XY model”, J. Phys. A 13 (1980) 585 | Wk 4 | the Kosterlitz flow beyond leading order |
| Pelissetto & Vicari, “Renormalization-group flow and asymptotic behaviors at the Berezinskii–Kosterlitz–Thouless transitions”, Phys. Rev. E 87 (2013) 032105 [arXiv:1212.2322] | Wk 4 | canonical form of the next-order flow; finite-size stiffness |
Committed 2026-07-01 as part of the Phase-1 scaffold; Block A additions appended 2026-07-07; corrections and additions from the 2026-09-27 review appended the same day. Per-week reading pointers live in the block skeletons.