Gauge Functors on a Finite Graph: The Holonomy Equivalence for Non-Abelian Gauge TheoryResearch Paper
Motivation
A gauge theory can be formulated in several mathematically different ways: with potentials (connections), with field strengths (curvature), or with holonomies, the parallel transports around closed loops. Philosophers and physicists ask whether these formulations say the same thing, and which one carries "surplus structure".
Category theory makes the question precise. Each formulation is a category of models, and each translation between formulations is a functor. A functor that is faithful and essentially surjective but not full forgets structure. One that is full and faithful but not essentially surjective forgets properties. One that is full and essentially surjective but not faithful forgets stuff. One that is all three forgets nothing and is an equivalence. This taxonomy is due to Baez, Bartels and Dolan (Baez–Shulman, §2.4).
Weatherall (2016) applied it to electromagnetism. Potentials without gauge arrows forget structure relative to field strengths (Proposition 1). The erratum in arXiv v2 (p. 15) corrects his Proposition 2: the principal-bundle formulation, whose arrows include gauge transformations, forgets only stuff, not nothing. Nguyen, Teh and Wells obtain the same verdict for the gauge-orbit functor (their Proposition 3.2.3). In their footnote 26 they identify the forgotten stuff as the constant ("global") gauge transformations. All of this is abelian, U(1) on a contractible spacetime.
The non-abelian counterpart is the holonomy formulation. Barrett's reconstruction and representation theorems, and their categorical upgrade by Rosenstock and Weatherall (Theorem 2), show that on a connected manifold, principal connections and generalized holonomy maps form equivalent categories. On the topological side, Freed and Quinn (eqs. 3.11–3.13) identify the automorphisms of a finite-group gauge field with a centralizer.
This mission states these results for an arbitrary group on a finite graph. There the smooth and topological subtleties disappear, but the categorical content survives intact.
Setting
A finite directed graph has vertices , edges , and maps . A step is an edge traversed forwards or backwards, and a walk is a list of steps whose endpoints chain. is connected from if every vertex is reached by a walk from .
- A connection is . Its holonomy along a walk is the ordered product of (forwards) and (backwards), as in Baez (1996), §2.
- A gauge transformation is , acting by .
- : objects are connections, and arrows are gauge transformations with . This is the discrete analogue of the groupoid of Nguyen–Teh–Wells.
- : a holonomy map at assigns a group element to each walk. It is multiplicative on loops at and unchanged when a backtrack is inserted into a loop at ; this is the discrete form of thin equivalence. Arrows are elements with on every loop at . Only values on loops at matter.
- Functors. sends and . sends to the discrete category of gauge orbits.
- Curvature. On a 2-complex, each face has a base vertex and a boundary loop. The curvature functor sends to the family of conjugacy classes of its face holonomies, which is the gauge-invariant non-abelian field strength.
Formalization targets
Goal: the holonomy functor is an equivalence
This is the discrete, fixed-base-point form of Rosenstock–Weatherall's Theorem 2. In the taxonomy above, potentials-with-gauge and holonomies forget nothing relative to each other. The statement holds for every group , finite or not. The base-point-changing arrows of Rosenstock–Weatherall are not included.
Milestones
- Faithful. A gauge arrow between two connections is determined by its value at .
- Full. Every conjugation relating the holonomy maps of and is realized by a gauge transformation.
- Barrett reconstruction. Every holonomy map at equals on all loops at , for some connection .
- Barrett representation. on loops at iff for a gauge transformation with , and that is unique.
- Stabilizer = centralizer. Evaluation at is a bijection from the gauge stabilizer of onto the centralizer of its holonomies at . This is the non-abelian , the discrete form of Freed–Quinn (3.11)–(3.13).
- The orbit functor forgets only stuff. It is full and essentially surjective. It is faithful iff has no vertices or is trivial. This is the discrete form of Nguyen–Teh–Wells Proposition 3.2.3 and of Weatherall's corrected Proposition 2.
- Aharonov–Bohm. Take nontrivial, abelian or not. On the boundary of a triangle, which has no faces, the curvature functor is not full: flat connections with different holonomy are not gauge-equivalent. On the filled triangle the curvature functor is full and essentially surjective but not faithful.
Significance
- Equivalence of formulations. The goal says that, once gauge transformations are arrows, the potential and holonomy formulations of non-abelian lattice gauge theory are categorically equivalent. This is the precise sense in which "the physics is in the holonomies".
- Stuff and global symmetry. Milestones 5–6 locate the forgotten stuff exactly. When potentials are compared with gauge-invariant data that lacks arrows, the stuff is the centralizer of the holonomy group, the global gauge symmetry that survives a choice of connection. In the abelian case this is Nguyen–Teh–Wells' footnote 26. In general it is the automorphism group that weights the Dijkgraaf–Witten / Freed–Quinn sum.
- Topology. Milestone 7 shows that on a non-simply-connected graph the curvature formulation also forgets structure. Weatherall's footnote 9 sets this situation aside for Minkowski space.
- Novelty. Each ingredient is classical in some setting. A machine-checked statement of the non-abelian classification on finite graphs, in the language of forgetful functors, does not appear to exist. It is a step towards treating the theories-as-categories programme formally.
Difficulty
- Combinatorics of walks. Lists of steps, their endpoint conditions, and the interaction of concatenation with backtracking all have to be handled explicitly. The goal and Milestones 1–4 need statements about walks between arbitrary vertices, not only loops.
- Essential surjectivity. Reconstruction has to produce a connection from data that is only constrained on loops at one vertex. Connectivity enters non-trivially.
- Faithfulness versus fullness. These use the hypotheses differently, and the boundary cases (empty graph, trivial group) have to be tracked.
- Milestone 7 needs explicit non-equivalences, and so a gauge invariant separating gauge orbits.
Formalization scope
- Graphs. These are finite directed graphs with
Fin-indexed cells and are not required to be simple. Loops and multiple edges are allowed. A 2-complex adds faces with a base vertex and a boundary walk proved to be a loop. - Groups. is any
Group; finiteness is not assumed. - Holonomy maps. These are functions on all lists of steps whose axioms only constrain loops at . Two maps agreeing on loops are isomorphic in (via ) but need not be equal. Reconstruction is therefore stated on loops.
- Functor properties. These are Mathlib's
Functor.Full,Functor.FaithfulandFunctor.EssSurj. The goal is their conjunction, not an explicitly constructed inverse. - Excluded. Spacetime symmetries (graph automorphisms), base-point-changing holonomy isomorphisms, and smooth or continuum statements are left out.
- Proved in the definitions. Gauge covariance of holonomy along walks is proved in the definitions file, because the functors require it.
Selected references
- J. O. Weatherall, "Understanding Gauge", Philosophy of Science 83 (2016) 1039–1049. arXiv:1505.02229. arXiv v2 includes the erratum to Proposition 2 (p. 15).
- J. Nguyen, N. J. Teh, L. Wells, "Why surplus structure is not superfluous", British Journal for the Philosophy of Science 71 (2020). arXiv:1712.01228
- S. Rosenstock, J. O. Weatherall, "A categorical equivalence between generalized holonomy maps on a connected manifold and principal connections on bundles over that manifold", J. Math. Phys. 57 (2016) 102902. arXiv:1504.02401
- D. S. Freed, F. Quinn, "Chern–Simons theory with finite gauge group", Comm. Math. Phys. 156 (1993) 435–472. arXiv:hep-th/9111004
- J. C. Baez, M. Shulman, "Lectures on n-categories and cohomology", in Towards Higher Categories, Springer (2010) 1–68. arXiv:math/0608420
- J. C. Baez, "Spin network states in gauge theory", Adv. Math. 117 (1996) 253–272. arXiv:gr-qc/9411007