Abstract
We construct a q-boson representation of the Zamolodchikov-Faddeev algebra whose structure function is given by the stochastic R matrix of \(U_q(A^{(1)}_n)\) introduced recently. The representation involves quantum dilogarithm type infinite products in the \(n(n-1)/2\)-fold tensor product of q-bosons. It leads to a matrix product formula of the stationary probabilities in the \(U_q(A_n^{(1)})\)-zero range process on a one-dimensional periodic lattice.
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Notes
We write \(K_\alpha \) with \(\alpha =(\alpha _1,\ldots , \alpha _n)\) as \(K_{\alpha _1,\ldots , \alpha _n}\) rather than \(K_{(\alpha _1,\ldots , \alpha _n)}\) for simplicity. A similar convention will also be used for \(g_\alpha (\zeta ), X_\alpha (\zeta )\) and \(Z_\alpha (\zeta )\).
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Acknowledgements
This work is supported by Grants-in-Aid for Scientific Research No. 15K04892, No. 15K13429 and No. 16H03922 from JSPS.
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Appendix A: Proof of Theorem 1
Appendix A: Proof of Theorem 1
We will use the same symbol \(\varphi (\beta ,\gamma )\) (3) to mean (3)\(|_{n \rightarrow n+1}\). Moreover, \(\sum _{1\le i < j \le n+1}\beta _i \gamma _j\) with \(\beta \in {\mathbb Z}_{\ge 0}^n, \gamma \in {\mathbb Z}_{\ge 0}^{n+1}\) will also be denoted by \(\varphi (\beta ,\gamma )\).
We are going to prove Theorem 1 by induction on n. The relation (15)\(|_{n=1}\) is valid since it is equivalent to (9)\(|_{n=1}\). (The case \(n=2\) has been shown in [16] by a method different from here.) Thus, our task in the sequel is to show (15)\(|_{n\rightarrow n+1}\) assuming (15)\(|_{n=n}\).
Lemma 7
Under the assumption (15) \(|_{n=n}\), the relation (15) \(|_{n\rightarrow n+1}\) follows from the equality
Proof
Substitute (19)\(|_{n \rightarrow n+1}\) into (15)\(|_{n\rightarrow n+1}\). Applying (13) on the LHS, we get
where the temporal notation \((i,j,k) := \mathbf{b}^i \mathbf{k}^j \mathbf{c}^k\) is used. The symbol \(\alpha ^+_i\) is defined by (17)\(|_{n \rightarrow n+1}\) and \(\beta ^+_i, \gamma ^+_i\) are similar. Thus, to prove \(\text {LHS}=\text {RHS}\), it is sufficient, though not a priori necessary, to show that the coefficients of \(X_t(\lambda )X_s(\mu )\) are equal for each choice of \(t,s \in {\mathbb Z}_{\ge 0}^n\) and \(\alpha , \beta \in {\mathbb Z}_{\ge 0}^{n+1}\). Explicitly, it reads
One can pull out the common factor \(\bigotimes _{i=1}^n\mathbf{k}^{\alpha ^+_i+\beta ^+_i}\) from this equality to the left. The result reads
Note that this further contains a common rightmost factor \(\bigotimes _{i=1}^n \mathbf{c}^{\beta _i}\) and a common leftmost factor \(\bigotimes _{i=1}^n\mathbf{b}^{t_i}\). Removing them leads to (39).\(\square \)
Lemma 8
The following identities hold:
Proof
These relations can easily be checked by means of the q-binomial theorem.\(\square \)
Lemma 9
The equality (39) is equivalent to
for any \(s \in {\mathbb Z}_{\ge 0}^n\) and \(\alpha \in {\mathbb Z}_{\ge 0}^{n+1}\).
Proof
Comparing the coefficient of the basis vector \(\bigotimes _{i=1}^n\mathbf{b}^{s_i-p_i}\mathbf{c}^{\alpha _i-p_i}\) of \(\mathcal {B}^{\otimes n}\) on the both sides of (39) by means of (40), it is translated into the equality of the coefficients
for any arrays of nonnegative integers \(\alpha =(\alpha _1, \ldots , \alpha _n,\alpha _{n+1}), s=(s_1,\ldots , s_n), p=(p_1,\ldots , p_n)\) such that \(p_i \le \min (s_i,\alpha _i)\) for all \(1 \le i \le n\). On the RHS of (43), we have introduced the notation
for later convenience. Of course \(\varphi (s^{\vee },\gamma ) = \varphi (s,\gamma )\) by the definition. By substituting (3) into (43) and removing a common overall factor from the both sides, it becomes
where \(\nu = \mu /\lambda \) and \(m^{\vee }, p^{\vee }\) are defined similar to (44). By the replacement
the above relation is cast into
which turns out to be free from \(p=(p_1,\ldots , p_n)\). This coincides with (42).\(\square \)
So far we have shown that Theorem 1 is a corollary of (42). Let us proceed to a proof of the latter.
Lemma 10
The equality (42) holds for \(n \in {\mathbb Z}_{\ge 0}\).
Proof
Again we invoke the induction on n. At \(n=0\), (42) reads \(1= \sum _{\gamma _1 \le \alpha _1} \Phi ^{(1)}_q(\gamma _1|\alpha _1;\lambda , \mu )\), which is indeed valid thanks to (9). Assume (42)\(|_{n\rightarrow n-1}\). Applying (11) to the LHS of (42)\(|_{n=n}\), we get
where \(\overline{m}, \overline{s} \in {\mathbb Z}_{\ge 0}^{n-1}\) and \(\overline{\alpha } \in {\mathbb Z}_{\ge 0}^n\) are defined by (10). Rewriting the sum over \(\overline{m}\) by the induction assumption (42)\(|_{n\rightarrow n-1}\) yields (\(\nu =\mu /\lambda \) as before)
where \(\xi (s,\overline{\alpha }, \overline{\gamma }) =\varphi (\overline{\gamma }, \overline{\alpha })+\varphi (\overline{s},\overline{\gamma }) +\sum _{i=2}^ns_i\gamma _i -\varphi (\overline{\gamma },\overline{\gamma })+ s_1|\overline{\gamma }|\). On the other hand, the RHS of (42) has been written out in the RHS of (45), which is expressed using the above \(\xi (s,\overline{\alpha }, \overline{\gamma })\) as
Denote the summand in (46) by \(\text {LHS}(m_1,\gamma _2,\ldots , \gamma _{n+1})\) and the one in (47) by \(\text {RHS}(\gamma _1,\gamma _2,\ldots , \gamma _{n+1})\). We claim \(\sum _{m_1\le s_1} \text {LHS}(m_1,\gamma _2,\ldots , \gamma _{n+1}) = \sum _{\gamma _1 \le \alpha _1} \text {RHS}(\gamma _1,\gamma _2,\ldots , \gamma _{n+1})\) holds for each fixed \(\overline{\gamma } = (\gamma _2,\ldots , \gamma _{n+1})\). In fact, the two sides possess a common overall factor \(q^{\xi (s,\overline{\alpha }, \overline{\gamma })} \nu ^{|\overline{\gamma }|} \frac{(\lambda )_{|\overline{\gamma }|} (\nu )_{|\overline{\alpha }|-|\overline{\gamma }|}}{(\mu )_{|\overline{\alpha }|}} \prod _{i=2}^{n+1}\left( {\begin{array}{c}\alpha _i\\ \gamma _i\end{array}}\right) _{q}\). By removing it, the claim becomes
This is simply stated as \(f(\alpha _1, s_1; q^{|\overline{\gamma }|}\lambda , q^{|\overline{\alpha }|}\mu ) = f(s_1, \alpha _1; q^{|\overline{\gamma }|}\lambda , q^{|\overline{\alpha }|}\mu )\) in terms of the function defined for \(s,t \in {\mathbb Z}_{\ge 0}\) and \(\nu =\mu /\lambda \) by
This is verified in Lemma 11.\(\square \)
Lemma 11
The function (48) enjoys the symmetry \(f(s,t;\lambda ,\mu ) = f(t,s;\lambda ,\mu )\) for \(s,t \in {\mathbb Z}_{\ge 0}\).
Proof
By applying (41) to the factor \(q^{si}\) in (48), \(f(s,t;\lambda , \mu )\) is rewritten as follows:
Replacing i by \(i+r\), we have
From \(\sum _{i=0}^{t-r} \Phi ^{(1)}_q(i|t-r;q^r\lambda , q^r\mu )=1\) (9), we find \(h(r,t;\lambda , \mu )=1\). Then the expression (49) tells that \(f(s,t;\lambda , \mu )=f(t,s;\lambda , \mu )\).\(\square \)
Proof of Theorem 1
As a summary of the arguments so far, the induction step from (15)\(|_{n=n}\) to (15)\(|_{n=n+1}\) has been established by the following scheme:
Since (15)\(|_{n=1}\) is valid as explained in the beginning of the appendix, the ZF relation (15) holds for any n. This completes the proof of Theorem 1. \(\square \)
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Kuniba, A., Okado, M. A q-boson representation of Zamolodchikov-Faddeev algebra for stochastic R matrix of \(\varvec{U_q(A^{(1)}_n)}\) . Lett Math Phys 107, 1111–1130 (2017). https://doi.org/10.1007/s11005-016-0934-7
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DOI: https://doi.org/10.1007/s11005-016-0934-7