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Theta function solutions of the qKZB equation for a face model
Mathematical Physics · Submitted 15 Sep 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We provide explicit solutions as theta functions.
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The abstract, sentence by sentence
We consider the quantum Knizhnik-Zamolodchikov-Bernard equation for a face model with elliptic weights, the SOS model. We provide explicit solutions as theta functions. On the so-called combinatorial line, in which the model is equivalent to the three-colour model, these solutions are shown to be eigenvectors of the transfer matrix with periodic boundary conditions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider the quantum Knizhnik-Zamolodchikov-Bernard equation for a face model with elliptic weights, the SOS model. | background 0.88 | 0.31 | 0.05 | asserted 0.84 |
| s1 | We provide explicit solutions as theta functions. | contribution 0.69 | 0.95 | 0.66 | asserted 1.00 |
| s2 | On the so-called combinatorial line, in which the model is equivalent to the three-colour model, these solutions are shown to be eigenvectors of the transfer matrix with periodic boundary conditions. | result 0.99 | 0.90 | 0.39 | asserted 1.00 |
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The paper
Original abstract
We consider the quantum Knizhnik-Zamolodchikov-Bernard equation for a face model with elliptic weights, the SOS model. We provide explicit solutions as theta functions. On the so-called combinatorial line, in which the model is equivalent to the three-colour model, these solutions are shown to be eigenvectors of the transfer matrix with periodic boundary conditions.
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What it cites · 17 sentences without a confident label
Compares with 4 papers
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In [ref] , the level $ℓ=1$ qKZ solutions were themselves constructed by computing matrix elements (as opposed to traces) of vertex operators between level-1 highest weight states [ref] .
Around the Razumov-Stroganov conjecture: proof of a multi-parameter sum rule · Discussion · 0.93
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Also, the solutions of [ref] are “hypergeometric integrals” in the sense that they generalise the generic hypergeometric solution of the KZ equation.
Solutions of the elliptic qKZB equations and Bethe ansatz I · Discussion · 0.99
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Furthermore, in the current work, we are able to provide explicit formulae for the entries of the solution of the qKZB system, leaving the inhomogeneities free – in [ref] , they were “half-specialised” to pairs of opposite values, resulting in expressions involving only even theta functions and therefore a rational parameterisation; here no such parameterisation is available.
Sum rule for the eight-vertex model on its combinatorial line · Discussion · 1.00
Cites as background 7 papers
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Generalising both the KZB and qKZ equations, Felder introduced the qKZB equations [ref] .
Conformal field theory and integrable systems associated with elliptic curves · Introduction · 0.83
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The equations satisfied by the inhomogeneous ground state turned out to be nothing but the qKZ system [ref] , and using related representation theory, an explicit form of the ground state entries was provided [ref] in terms of certain contour integrals.
Quantum Knizhnik-Zamolodchikov equation, generalized Razumov-Stroganov sum rules and extended Joseph polynomials · Introduction · 0.85
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The equations satisfied by the inhomogeneous ground state turned out to be nothing but the qKZ system [ref] , and using related representation theory, an explicit form of the ground state entries was provided [ref] in terms of certain contour integrals.
Polynomial solutions of qKZ equation and ground state of XXZ spin chain at Delta = -1/2 · Introduction · 0.85
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