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In mathematics, a Casimir element (also known as a Casimir invariant or Casimir operator) is a distinguished element of the center of the universal enveloping algebra of a Lie algebra. A prototypical example is the squared angular momentum operator, which is a Casimir element of the three-dimensional rotation group.
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| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Casimir element | related to Casimir elements and representation theory | By Racah's | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | Lie | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | The Casimir | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | Laplacian | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | By | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | By Schur's Lemma | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | Casimir | 0.60 | section |
| Casimir element | related to Casimir elements and representation theory | The | 0.60 | section |
| Casimir element | related to Relation to the Laplacian on G | If | 0.60 | section |
| Casimir element | related to Relation to the Laplacian on G | Lie | 0.60 | section |
| Casimir element | related to Relation to the Laplacian on G | Riemannian | 0.60 | section |
| Casimir element | related to Relation to the Laplacian on G | Then | 0.60 | section |
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