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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 on , with the two possible orientations.
Riemannian hodge star: On an oriented Riemannian -manifold, for the Hodge star is the fibrewise map characterized by for every pair of -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 , it multiplies by the chosen orientation sign.
Hodge star is a smooth bundle isomorphism: The Hodge star exists uniquely and is a smooth bundle isomorphism in every degree .
Refutation
With positive orientation the volume form is ; with negative orientation it is . In degree zero, , so the defining identity gives and . Both are the stars for their respective oriented metrics.
The one-form 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.
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
5 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- John M. Lee, Introduction to Smooth Manifolds, second edition (standard reference, not scraped)