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In mathematics, the Hodge star operator or Hodge star is a linear map defined on the exterior algebra of a finite-dimensional oriented vector space endowed with a nondegenerate symmetric bilinear form. Applying the operator to an element of the algebra produces the Hodge dual of the element. This map was introduced by W. V. D. Hodge.
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| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Hodge star operator | is a | linear operator on the exterior algebra of V | 0.90 | text |
| Hodge star operator | is a | case n | 0.90 | text |
| pseudo-Riemannian manifolds | instance of | In more general contexts | 0.80 | text |
| Minkowski space | instance of | In more general contexts | 0.80 | text |
| the bilinear form may not be positive-definite | instance of | In more general contexts | 0.80 | text |
| spinor-helicity formalism or twistor theory.Conformal invarianceThe Hodge star is conformally invariant on n-forms on a 2n-dimensional vector space V | instance of | making contacts to the use of the two-spinor language in modern physics | 0.80 | text |
| spinor-helicity formalism or twistor theory | instance of | making contacts to the use of the two-spinor language in modern physics | 0.80 | text |
| Hodge star operator | related to Four dimensions | In | 0.60 | section |
| Hodge star operator | related to Four dimensions | Hodge | 0.60 | section |
| Hodge star operator | related to Four dimensions | If | 0.60 | section |
| Hodge star operator | related to Four dimensions | Riemannian | 0.60 | section |
| Hodge star operator | related to Four dimensions | Duality | 0.60 | section |
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