Hopf theory MOC

Casimir invariant of a Hopf 𝕂-algebra

Let H be a finite-dimensional Hopf 𝕂-algebra equipped with an invariant bilinear form 𝐡. Let 𝑅 ≀HadH be an H-submodule upon which 𝐡 is nondegenerate, so that πœ” βˆˆπ‘… βŠ—π‘… is a coΓ«valuation. Then the Casimir invariant

Ω𝑅,𝐡=πœ‡(πœ”)

is in the centre of H.1 #m/thm/hopf In terms of string diagrams, Ω𝑅,𝐡 may be written as

c

Proof

We adopt the Einstein summation convention.

In light of Centre of a Hopf algebra as H-invariants, it suffices to show Ξ© :=Ω𝑀,𝐡 satisfies

π‘₯β–ΉΞ©=πœ–(π‘₯)Ξ©

for all π‘₯ ∈H. Suppose πœ” =𝑣𝑖 βŠ—π‘£π‘–. Applying ^P2 we have

π‘₯β–ΉΞ©=π‘₯β–Ή(𝑣𝑖𝑣𝑖)=βˆ‘(π‘₯)(π‘₯(1)▹𝑣𝑖)(π‘₯(2)▹𝑣𝑖)=βˆ‘(π‘₯)βŸ¨π‘£π‘—,π‘₯(1)β–Ήπ‘£π‘–βŸ©βŸ¨π‘₯(2)▹𝑣𝑖,π‘£π‘˜βŸ©π‘£π‘—π‘£π‘˜=βˆ‘(π‘₯)βŸ¨π‘£π‘—,π‘₯(1)β–Ήπ‘£π‘–βŸ©βŸ¨π‘£π‘–,𝜎(π‘₯(2))β–Ήπ‘£π‘˜βŸ©π‘£π‘—π‘£π‘˜=βˆ‘(π‘₯)βŸ¨π‘£π‘—,π‘₯(1)β–ΉπœŽ(π‘₯(2))β–Ήπ‘£π‘˜βŸ©π‘£π‘—π‘£π‘˜=βˆ‘(π‘₯)βŸ¨π‘£π‘—,π‘₯(1)𝜎(π‘₯(2))β–Ήπ‘£π‘˜βŸ©π‘£π‘—π‘£π‘˜=πœ–(π‘₯)βŸ¨π‘£π‘—,π‘£π‘˜βŸ©π‘£π‘—π‘£π‘˜=πœ–(π‘₯)Ξ©

as required.


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Footnotes

  1. 1992. Casimir invariants for Hopf algebras ↩