Weyl integral

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Let π’ž=(π’ž,βŠ—,I) be a (strict) monoidal category. The centre of π’ž, denoted 𝒡(π’ž), is the category whose objects are pairs (A,u) consisting of an object A of π’ž and a natural isomorphism uX:AβŠ—Xβ†’XβŠ—A satisfying

uXβŠ—Y=(1βŠ—uY)(uXβŠ—1)

and

uI=1A (this is actually a consequence of the first axiom).

An arrow from (A,u) to (B,v) in 𝒡(π’ž) consists of an arrow f:Aβ†’B in π’ž such that

vX(fβŠ—1X)=(1XβŠ—f)uX .

The category 𝒡(π’ž) becomes a braided monoidal category with the tensor product on objects defined as

(A,u)βŠ—(B,v)=(AβŠ—B,w)

where wX=(uXβŠ—1)(1βŠ—vX), and the obvious braiding .

References

AndrΓ© Joyal and Ross Street. Tortile Yang-Baxter operators in tensor categories, J. Pure Appl. Algebra 71 (1991): 43–51.


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