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The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
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These labels describe origin, not correctness: citations and verification chips remain separate evidence.
A transverse local gauge condition gives a second-class slice
Local slice near a point where the gauge matrix is invertible; no uniqueness for distant orbits.
Statement
Let be regular first-class constraints on as in Regular first-class constraints admit local symplectic reduction, and choose a point . Let be smooth functions with and suppose is invertible at . By continuity, it remains invertible on a neighborhood of in . Then the combined constraint matrix for is invertible near , so the combined surface is second class and carries the Dirac symplectic form. After shrinking the neighborhood, each nearby characteristic leaf intersects the gauge surface in exactly one point within that coordinate neighborhood. This is a local slice assertion only. When the characteristic leaves are points and the empty gauge condition is immediate; the proof below treats .
Facts & Assumptions
Given: A regular first-class constraint surface, smooth gauge functions, and an invertible transverse bracket matrix near the chosen point.
The Axiom of Countable Choice (): Assume countable choice ACω, meaning every sequence of nonempty sets has a choice function; no full Axiom of Choice is assumed.
Regular first-class constraints admit local symplectic reduction: the independent characteristic fields span a smooth rank- involutive distribution with local leaf coordinates.
Second-class constraints and the Dirac bracket: invertible constraint bracket matrix implies an embedded symplectic joint level with Dirac bracket.
Choice-free smooth inverse function theorem in Euclidean space: a smooth map between equal-dimensional Euclidean open sets with invertible derivative at a point is a diffeomorphism between suitable neighborhoods.
Proof
On the common zero set, the combined matrix has block form , where there by first-classness and . If it annihilates , its first block equation is , so ; its second is , so . Thus it is invertible; continuity preserves invertibility on a smaller neighborhood.
[F2] applied to the combined list makes its zero surface embedded and symplectic with the displayed Dirac bracket.
In Frobenius coordinates from [F1] around , use the local frame along each leaf. At , its derivative on the gauge map has entries , so it is invertible; changing to the -coordinate frame multiplies by an invertible matrix. For , [F3] therefore gives a local diffeomorphism of the gauge map along each leaf.
At the gauge map has value by the statement. Consider the equal-dimensional map . Its derivative at is block triangular with invertible diagonal blocks by step 2.2 and the identity on . Applying [F3] gives a neighborhood on which this map is a diffeomorphism; therefore, for each nearby , the gauge equations have exactly one local solution . This proves exactly one intersection within that product neighborhood, with no claim about distant portions of a leaf.