Definition

Let g\mathfrak g be a finite-dimensional over R\mathbb R or C\mathbb C, let BB be its , and choose bases (Xi)(X_i) and (Xi)(X^i) dual with respect to BB. The Casimir element in the is

ΩB=iXiXiU(g).\Omega_B=\sum_i X_iX^i\in U(\mathfrak g).

ΩB\Omega_B is independent of the chosen dual bases and belongs to . If a representation dπd\pi of g\mathfrak g is extended to U(g)U(\mathfrak g), then dπ(ΩB)d\pi(\Omega_B) is its Casimir operator.

Centrality and normalization

The invariance of BB makes the tensor corresponding to the identity map on g\mathfrak g invariant under the adjoint action; multiplication into U(g)U(\mathfrak g) therefore makes ΩB\Omega_B central. Replacing BB by cBcB replaces ΩB\Omega_B by c1ΩBc^{-1}\Omega_B, 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 g\mathfrak g-action, it is a module endomorphism. On an irreducible complex representation in a setting where gives scalar endomorphisms, it acts by a scalar. For highest-weight modules this scalar can be computed from the and the half-sum of ; the formula changes with the normalization of BB.

Conventions and scope

For a real semisimple Lie algebra, one often forms the element after complexifying g\mathfrak g. More generally, any nondegenerate invariant symmetric 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
  1. Anthony W. Knapp, Lie Groups Beyond an Introduction, 2nd ed., Birkhäuser, 2002. DOI record. Relevant: Chapter V, §5 on the center and Casimir element.
  2. 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.