Abstract
An expression for the R-matrix associated with \({\mathcal {U}}_q({\widehat{\mathfrak e_8}})\) in its 249-dimensional representation is given using the diagrammatic calculus of \({\mathcal {U}}_q({\mathfrak {e}_8})\) invariants.
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Notes
Note that these identities do depend on the choice of normalization of B and T, which is determined by imposing that it agrees with the standard \({\mathfrak {e}_8}\) convention at \(q=1\), that it be the simplest possible (entries are coprime polynomials) and that constants occurring in the identities be palindromic in q (which fixes the remaining freedom of multiplying by a power of q).
Note in particular that the “multiplicity-free” property that is crucial in e.g. [5] fails here.
Requiring both unitarity and crossing relations without a prefactor would take us beyond the realm of rational functions, and we do not pursue this here.
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PZJ was supported by ARC Grants FT150100232 and DP180100860. He would like to thank A. Kuniba for useful discussions and J. Lamers for comments on the manuscript.
Appendices
Appendix A Some product rules
Appendix B The main formula
Appendix C Rational limit
The rational R-matrix is obtained from the trigonometric one in the correlated limit \(q,z\rightarrow 1\):
Representation theoretically, it corresponds to the limit from the quantized loop algebra \({\mathcal {U}}_q({\mathfrak {e}_8}[z^\pm ])\) (i.e., the quotient of \({\mathcal {U}}_q({\widehat{\mathfrak e_8}})\) by \(\prod _{i=0}^8 k_i^{n_i}=1\)) to the Yangian \(\mathcal Y({\mathfrak {e}_8})\cong {\mathcal {U}}_q({\mathfrak {e}_8}[z])\). In this Appendix, we show briefly how to recover the results of [12].
The main simplification in the diagrammatic calculus (see the related discussion at the start of Sect. 3.3) is that undercrossings and overcrossings become indistinguishable:
and both become equal to the naive permutation of tensors of \(V\otimes V\). The reader is invited to write the simplified relations that diagrams satisfy in this limit; we only provide one example:
The expression of the R-matrix in Appendix B becomes in the rational limit:
The alternative basis of Sect. 3.3 no longer makes sense because and are degenerate; we can however use an intermediate basis, in which the R-matrix becomes
the other terms (involving empty vertices) remaining the same.
It is not hard to see that the latter result coincides with that of [12] (see the equation between (3.9) and (3.10)), being careful that the expression there is \(R(w)=P\check{R}_{\text {rat}}(x=-w)\) where P is permutation of factors, on condition that the following normalizing factor is used:
with the substitution \(i\hbar \rightarrow \hbar \) and with the free parameter \(\alpha \) (which is related to our parameter \(\kappa \)) given the value
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Zinn-Justin, P. The trigonometric \(E_8\) R-matrix. Lett Math Phys 110, 3279–3305 (2020). https://doi.org/10.1007/s11005-020-01330-9
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DOI: https://doi.org/10.1007/s11005-020-01330-9