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Physics theoremStatement: AI-adaptedProof: AI-generatedPipeline-generatedprecheck passverified 2026-11-05 (gpt-6.1-sol)
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Coordinate invariance of the local Beltrami antighost pairing

Physical scope

Local tensorial coordinate covariance of the bosonic bc/Beltrami pairing on an overlap; it supplies no global gauge slice or determinant line.

Statement

Let z and w=f(z) be holomorphic coordinates with f′(z)≠0 on an overlap. If b=bzz(z)dz2 is the antighost quadratic differential and μ=μzˉ zdzˉ⊗∂z is a Beltrami differential, then the local density bzzμzˉ zdx dy is invariant under this coordinate change. Hence, for compactly supported local data, (b,μ)=∫bzzμzˉ zdx dy is independent of the chosen holomorphic chart.

Facts & Assumptions

Given: A complex coordinate overlap w=f(z) with nonvanishing derivative and compactly supported local b,μ.

[F1]

Bosonic Bc Ghost System: b has holomorphic conformal weight 2 and transforms as a quadratic differential. The Beltrami tensor type is the explicit hypothesis μ=μzˉ zdzˉ⊗∂z in the Statement, not a conclusion of this ghost supplier.

Proof

1.1givenF1algebra

By [F1], bww=bzz(dz/dw)2=bzz/f′(z)2. For the tensor μ specified in the Statement, dzˉ=dwˉ/f′(z)‾ and ∂z=f′(z)∂w, so μwˉ w=f′(z)μzˉ z/f′(z)‾. The area elements satisfy dxwdyw=∣f′(z)∣2dxzdyz.

2.1step 1.1algebra∎

Multiplying these three factors gives bwwμwˉ wdxwdyw=bzzf′2f′f′‾ ∣f′∣2dxzdyz=bzzμzˉ zdxzdyz. Because the support is compact and the density agrees pointwise on each overlap, a partition into coordinate patches gives the same integral in either atlas. No statement about a global gauge slice or determinant trivialization follows.

Depends on

Dependency tree · 2 levels

Sources