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False statementConstruction: AI-adaptedVerification: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-10
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The hodge star is defined without an orientation

Statement

The ordinary Hodge star is determined by the Riemannian metric without any orientation.

Facts & Assumptions

Given: The same Euclidean metric dx2 on R, with the two possible orientations.

[F1]

Riemannian hodge star: On an oriented Riemannian n-manifold, for 0kn the Hodge star is the fibrewise map :kTMnkTM characterized by αβ=α,βgvolg for every pair of k-covectors. The pairing is the determinant-normalized one of prop-riemannian-metrics-induce-metrics-on-dual-tensor-and-exterior-bundles, and the positive unit volume form is prop-the-riemannian-volume-form-is-the-unique-positive-unit-top-form. This is the ordinary, orientation-dependent star, with no orientation-line twist. Existence, uniqueness and smoothness are proved in thm-hodge-star-is-a-smooth-bundle-isomorphism. For n=k=0, it multiplies by the chosen orientation sign.

[F2]

Hodge star is a smooth bundle isomorphism: The Hodge star exists uniquely and is a smooth bundle isomorphism in every degree 0kn.

Refutation

technique · direct
1.1

With positive orientation the volume form is dx; with negative orientation it is dx. In degree zero, 1,1=1, so the defining identity 11=1,1vol gives +1=dx and 1=dx. Both are the stars for their respective oriented metrics.

F1F2given
2.1

The one-form dx is nonzero, so the two results differ, although the underlying metric is identical. Hence that metric alone cannot specify the ordinary Hodge star; the claimed orientation independence fails already in dimension one.

step 1.1

Source locator

Lee, Problem 16-18(a–c), pp. 437–438, Hodge star on oriented inner-product spaces; the one-dimensional orientation reversal is calculated above.

Depends on

Used by

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Dependency tree · two levels

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Sources