Theorem
Slice theorem for the gauge action
A local normal-form theorem modeling a neighborhood of a gauge orbit by a Coulomb slice modulo the connection stabilizer.
Statement
Let be a principal bundle with compact structure group over a closed Riemannian -manifold. Use the Sobolev completions of connections in and gauge transformations in , with . For a connection , there is such that the Coulomb slice
meets every sufficiently nearby gauge orbit. Moreover, a neighborhood of the orbit of in the connection space is modeled equivariantly by
Why the Coulomb condition is transverse
The tangent to the gauge orbit at is , while selects its -orthogonal complement. Solving for a gauge transformation that places in the slice reduces, after linearization, to the elliptic operator . The implicit-function theorem then supplies existence and local uniqueness up to the stabilizer of Freed–Uhlenbeck, Theorem 3.4.
The offset in Sobolev regularity is essential: a gauge transformation acts on a connection without losing a derivative. The hypothesis provides the multiplication and continuity properties required by the nonlinear action.
Quotient structure
Passing to the quotient gives a local model
for the moduli problem near . If the stabilizer acts trivially after central symmetries are removed, this behaves like a Banach-manifold chart. A nontrivial stabilizer produces an orbifold-type or more singular local quotient. Thus the theorem explains why irreducible connections form the regular stratum and reducible connections create singular strata.
Conventions and scope
References
- Daniel S. Freed and Karen K. Uhlenbeck, Instantons and Four-Manifolds, 2nd ed., Springer, 1991. DOI record. Relevant: Chapter 3, especially Theorem 3.4, the slice theorem for the gauge action.
- Simon K. Donaldson and Peter B. Kronheimer, The Geometry of Four-Manifolds, Oxford University Press, 1990. DOI record. Relevant: §4.2, Sobolev gauge groups and local slices.