Gribov Ambiguity: no continuous gauge fixing (Singer 1978)Research Paper
Motivation
In the Feynman path-integral approach to a non-abelian gauge theory one wants to integrate a gauge-invariant weight over the space of vector potentials (connections) of a principal bundle. The integrand is constant on the orbits of the group of gauge transformations, so the integral over diverges and one is supposed to integrate instead over the orbit space . The Faddeev–Popov procedure realizes this by fixing a gauge: choosing, continuously in the orbit, exactly one vector potential on each orbit, and correcting by a Jacobian determinant.
V. N. Gribov (SLAC Translation 176, 1977) observed that for potentials on (or ) with suitable conditions at infinity, the Coulomb gauge condition does not do this: the Coulomb slice through the zero potential meets the orbit of the zero potential again, far from the origin. These extra intersections are the Gribov copies; R. Jackiw, I. Muzinich and C. Rebbi (Phys. Rev. D 17 (1978) 1576) analyzed them in detail.
I. M. Singer, Some Remarks on the Gribov Ambiguity (Commun. Math. Phys. 60 (1978) 7–12), showed that the phenomenon is not a defect of the Coulomb gauge. If the conditions at infinity are those of Gribov — gauge transformations extending to the one-point compactification with value at infinity, so that the base manifold is or — then no continuous gauge fixing exists at all, in any gauge. The obstruction is topological: the space of irreducible connections is weakly contractible, while the gauge group is not, and a weakly contractible principal bundle admits no global continuous section.
Setting
Fix and take the structure group , the group of complex matrices with and , topologized as a subspace of matrices. Let denote the unit sphere of , with base point the north pole.
For the trivial -bundle over a space , a gauge transformation is a map , and the gauge group is
continuous maps with pointwise multiplication and the compact-open topology. Two subobjects matter. The based gauge group is the subgroup of transformations that are the identity at the base point. The constant transformations with value in the centre of form a normal subgroup, and the reduced gauge group is the quotient
with the quotient topology. The centre acts trivially on vector potentials, so is the group that acts effectively.
A group acting continuously on a space has orbit space with the quotient topology, and a gauge fixing is a continuous map with , where is the projection: a continuous choice of exactly one point on each orbit. The action is principal when it is free and the division map, which sends a pair of points on one orbit to a group element carrying the second to the first, can be chosen continuously; this is the topological content of " is a principal -bundle". The space is weakly contractible when it is nonempty and all its homotopy groups vanish.
In the paper, is the affine space of connections, its set of irreducible members, and Theorems 1 and 2 say exactly that is a weakly contractible principal -space.
Formalization targets
Goal — Corollary 4 (no gauge fixing)
For , , and every weakly contractible principal -space :
By Theorems 1 and 2 of the paper the space of irreducible connections over or is such an , so the goal contains Singer's Corollary 4 for that space; it leaves the analytic construction of the space of connections unfixed, which is what makes it statable today.
Milestone level — Theorem 3
Milestone level — Theorem 5 and its homotopy inputs
Significance
The result rules out the existence of a global gauge in the topological sense: every gauge condition used in practice is at best a local slice, and the Faddeev–Popov construction has to be read as a local statement, patched with a partition of unity over the orbit space (as the last section of the paper proposes). It is the mathematical reason why the Gribov ambiguity cannot be repaired by a cleverer gauge condition, and it is the origin of the Gribov–Zwanziger restriction of the functional integral to a fundamental domain.
Formalizing it adds a machine-checked version of an argument that is quoted far more often than it is checked, and it forces into Lean a piece of infrastructure that Mathlib currently lacks: homotopy groups of mapping spaces, the long exact sequence of a fibration in the form needed for , and the classical computations , for , . Singer's results are proved mathematics; none of them is formalized, and Mathlib as of the pinned revision contains homotopy groups as a definition together with their group structure, but essentially no computation of them.
Difficulty
The naive approach to the goal — build a section by hand, or average over the group — fails because is neither compact nor contractible and the obstruction is global: locally, slices do exist (that is the content of the generalized Coulomb gauge), so no local argument can produce a contradiction. The proof has to convert a section into a homotopy-theoretic statement: a section of a principal bundle trivializes it, exhibiting the group as a retract of the total space, so all homotopy groups of the group would vanish; the work is then to show that some homotopy group of the reduced gauge group does not vanish, which needs the identification of the based gauge group with a mapping space, the exact sequences relating , and , and non-trivial homotopy groups of — including for the case of Theorem 3.
Formalization scope
The formalization commits to the following conventions, all of them visible in the definitions of this mission.
- The bundle is the trivial -bundle, so gauge transformations are literally maps . This is the case of Gribov's original setting over ; over the paper also treats bundles of nonzero Pontrjagin index, which are out of scope here.
- Gauge transformations are continuous, not smooth, with the compact-open topology; Singer's Theorem 5 uses smoothing homotopies to pass between the two, and the homotopy-theoretic content is the same.
- is the special unitary group of complex matrices, with its subspace topology; is the unit sphere of with its subspace topology.
- Homotopy groups are Mathlib's
HomotopyGroup, based at the identity element. - The space of connections is not constructed: Mathlib has no space of connections on a principal bundle, and building one is a mission of its own. The goal therefore quantifies over an arbitrary topological space carrying a weakly contractible principal action of the reduced gauge group — exactly the properties Theorems 1 and 2 establish for the irreducible connections.
- This quantification is not vacuous: such spaces exist (the total space of a universal -bundle is one), so the goal is a genuine non-existence statement and not a statement about an empty class. Conversely it is not trivially true: the hypotheses do not mention any homotopy invariant of the gauge group, and refuting a section requires Theorem 3.
- The paper's analytic statements — Theorem 1 (openness and density of the irreducible connections, principal bundle structure), Theorem 2 (weak contractibility), Theorem 6 ( of the irreducible orbit space), Theorem 7 (no flat connection), Theorem 8 (tangency of orbits to the Coulomb slice) and Theorem 9 (the canonical connection and its curvature) — are out of scope until a space of connections exists in Lean. Contributions that build one, in reusable form, are welcome and would let this mission be extended to them.
Selected references
- V. N. Gribov, Instability of non-abelian gauge theories and impossibility of choice of Coulomb gauge, SLAC Translation 176 (1977); Nucl. Phys. B 139 (1978) 1–19, doi:10.1016/0550-3213(78)90175-X.
- I. M. Singer, Some Remarks on the Gribov Ambiguity, Commun. Math. Phys. 60 (1978) 7–12, doi:10.1007/BF01609471.
- R. Jackiw, I. Muzinich, C. Rebbi, Coulomb gauge description of large Yang-Mills fields, Phys. Rev. D 17 (1978) 1576, doi:10.1103/PhysRevD.17.1576.
- H. Toda, Composition methods in homotopy groups of spheres, Annals of Mathematics Studies 49, Princeton University Press (1962).