Statement

Let PMP\to M be a with compact structure group over a closed Riemannian nn-manifold. Use the of connections in Wk,pW^{k,p} and in Wk+1,pW^{k+1,p}, with kp>nkp>n. For a connection AA, there is ε>0\varepsilon>0 such that the

SA,ε={A+adAa=0, aWk,p<ε}\mathcal S_{A,\varepsilon} =\{A+a\mid d_A^*a=0,\ \|a\|_{W^{k,p}}<\varepsilon\}

meets every sufficiently nearby gauge orbit. Moreover, a neighborhood of the orbit of AA in the connection space is modeled equivariantly by

G×Stab(A)SA,ε.\mathcal G\times_{\operatorname{Stab}(A)}\mathcal S_{A,\varepsilon}.
Why the Coulomb condition is transverse

The tangent to the gauge orbit at AA is imdA\operatorname{im}d_A, while dAa=0d_A^*a=0 selects its L2L^2-orthogonal complement. Solving for a gauge transformation that places A+aA+a in the slice reduces, after linearization, to the elliptic operator dAdAd_A^*d_A. The implicit-function theorem then supplies existence and local uniqueness up to the Freed–Uhlenbeck, Theorem 3.4.

The offset in Sobolev regularity is essential: a Wk+1,pW^{k+1,p} gauge transformation acts on a Wk,pW^{k,p} connection without losing a derivative. The hypothesis kp>nkp>n provides the multiplication and continuity properties required by the nonlinear action.

Quotient structure

Passing to the quotient gives a local model

SA,ε/Stab(A)\mathcal S_{A,\varepsilon}/\operatorname{Stab}(A)

for the moduli problem near [A][A]. 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 form the regular stratum and create singular strata.

Conventions and scope
References
  1. 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.
  2. 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.