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On endomorphisms of quantum tensor space

Representation Theory 2008-06-25 v1 Mathematical Physics math.MP

Abstract

We give a presentation of the endomorphism algebra \End\cUq(\fsl2)(Vr)\End_{\cU_q(\fsl_2)}(V^{\otimes r}), where VV is the 3-dimensional irreducible module for quantum \fsl2\fsl_2 over the function field \C(q1/2)\C(q^{{1/2}}). This will be as a quotient of the Birman-Wenzl-Murakami algebra BMWr(q):=BMWr(q4,q2q2)BMW_r(q):=BMW_r(q^{-4},q^2-q^{-2}) by an ideal generated by a single idempotent Φq\Phi_q. Our presentation is in analogy with the case where VV is replaced by the 2- dimensional irreducible \cUq(\fsl2)\cU_q(\fsl_2)-module, the BMW algebra is replaced by the Hecke algebra Hr(q)H_r(q) of type Ar1A_{r-1}, Φq\Phi_q is replaced by the quantum alternator in H3(q)H_3(q), and the endomorphism algebra is the classical realisation of the Temperley-Lieb algebra on tensor space. In particular, we show that all relations among the endomorphisms defined by the RR-matrices on VrV^{\otimes r} are consequences of relations among the three RR-matrices acting on V4V^{\otimes 4}. The proof makes extensive use of the theory of cellular algebras. Potential applications include the decomposition of tensor powers when qq is a root of unity.

Keywords

Cite

@article{arxiv.0806.3807,
  title  = {On endomorphisms of quantum tensor space},
  author = {G. I. Lehrer R. B. Zhang},
  journal= {arXiv preprint arXiv:0806.3807},
  year   = {2008}
}

Comments

14 pages

R2 v1 2026-06-21T10:53:41.040Z