Definition
Casimir element and Casimir operator
A basis-independent central element of an enveloping algebra and the operator through which it acts in a representation.
Definition
Let be a finite-dimensional semisimple Lie algebra over or , let be its Killing form, and choose bases and dual with respect to . The Casimir element in the universal enveloping algebra is
is independent of the chosen dual bases and belongs to the center of . If a representation of is extended to , then is its Casimir operator.
Centrality and normalization
The invariance of makes the tensor corresponding to the identity map on invariant under the adjoint action; multiplication into therefore makes central. Replacing by replaces by , so numerical Casimir eigenvalues depend on the normalization of the invariant form Knapp, Chapter V, §5.
Action in representations
Because the Casimir operator commutes with the -action, it is a module endomorphism. On an irreducible complex representation in a setting where Schur's lemma gives scalar endomorphisms, it acts by a scalar. For highest-weight modules this scalar can be computed from the highest weight and the half-sum of positive roots; the formula changes with the normalization of .
Conventions and scope
For a real semisimple Lie algebra, one often forms the element after complexifying . More generally, any nondegenerate invariant symmetric bilinear form produces a quadratic Casimir element by the same construction. “Casimir invariant” may also refer to the scalar eigenvalue or to higher-degree central elements, so it is not always synonymous with this quadratic element.
References
- Anthony W. Knapp, Lie Groups Beyond an Introduction, 2nd ed., Birkhäuser, 2002. DOI record. Relevant: Chapter V, §5 on the center and Casimir element.
- Jacques Dixmier, Enveloping Algebras, Graduate Studies in Mathematics 11, American Mathematical Society, 1996. DOI record. Relevant: Chapters 2 and 7 on enveloping algebras and their centers.