Question

Check that the Boltzmann weights (7.153) for the chiral Potts model satisfy the Yang-Baxter equation (7.151) provided all the rapidities $p, q$ and $r$ lie on the same spectral manifold $\Gamma_\kappa$ (7.156). In order to do so, perform first the Fourier transform of the weights (7.153) with respect to $\sigma_3$, and introduce $$ \begin{aligned} V_{a b} & =\sum_{k=1}^N \omega^{b k} W_{p r}(a+k) \bar{W}_{q r}(k) \\ \bar{V}_{a b} & =\sum_{k=1}^N \omega^{a k} \bar{W}_{p r}(k) W_{q r}(b+k) \end{aligned} $$ The proof of (7.151) follows from the remark that the product formulae in (7.153) are equivalent to a pair of linear recurrence relations for both $V_{a b}$ and $\bar{V}_{a b}$.

    Check that the Boltzmann weights (7.153) for the chiral Potts model satisfy the Yang-Baxter equation (7.151) provided all the rapidities $p, q$ and $r$ lie on the same spectral manifold $\Gamma_\kappa$ (7.156). In order to do so, perform first the Fourier transform of the weights (7.153) with respect to $\sigma_3$, and introduce

$$
\begin{aligned}
V_{a b} & =\sum_{k=1}^N \omega^{b k} W_{p r}(a+k) \bar{W}_{q r}(k) \\
\bar{V}_{a b} & =\sum_{k=1}^N \omega^{a k} \bar{W}_{p r}(k) W_{q r}(b+k)
\end{aligned}
$$


The proof of (7.151) follows from the remark that the product formulae in (7.153) are equivalent to a pair of linear recurrence relations for both $V_{a b}$ and $\bar{V}_{a b}$.

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Quantum Groups in Two-Dimensional Physics
Quantum Groups in Two-Dimensional Physics
Cisar Gómez, Martm… 1st Edition
Chapter 7, Problem 10 ↓

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151) that we need to verify: $$\sum_{\sigma_3} W_{pq}(\sigma_1-\sigma_3) W_{pr}(\sigma_3-\sigma_2) W_{qr}(\sigma_1-\sigma_2) = \sum_{\sigma_3} W_{qr}(\sigma_3-\sigma_2) W_{pr}(\sigma_1-\sigma_3) W_{pq}(\sigma_1-\sigma_2)$$  Show more…

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Check that the Boltzmann weights (7.153) for the chiral Potts model satisfy the Yang-Baxter equation (7.151) provided all the rapidities $p, q$ and $r$ lie on the same spectral manifold $\Gamma_\kappa$ (7.156). In order to do so, perform first the Fourier transform of the weights (7.153) with respect to $\sigma_3$, and introduce $$ \begin{aligned} V_{a b} & =\sum_{k=1}^N \omega^{b k} W_{p r}(a+k) \bar{W}_{q r}(k) \\ \bar{V}_{a b} & =\sum_{k=1}^N \omega^{a k} \bar{W}_{p r}(k) W_{q r}(b+k) \end{aligned} $$ The proof of (7.151) follows from the remark that the product formulae in (7.153) are equivalent to a pair of linear recurrence relations for both $V_{a b}$ and $\bar{V}_{a b}$.
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