Abstract
In this paper we prove that the Euler–Lagrange equations for the limit shape for the inhomogeneous six vertex model on a cylinder have infinitely many conserved quantities.
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Notes
The idea of using a superposition of plane waves as an eigenfunction for the Heisenberg spin Hamiltonian (which is the the logarithmic derivative of the transfer-matrix of the homogeneous 6-vertex model at \(u=0\)) goes back to H. Bethe [B]. It was first applied to the 6-vertex model by E. Lieb in [L] for zero magnetic fields. Shorty after C.P. Yang [Y] applied it to the asymmetric 6-vertex model (with magnetic fields). The algebraic form we use is due to L. Faddeev and L. Takhtajan [FT2].
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Acknowledgements
The work of N.R. was partly supported by Grants NSF FRG DMS-1664521 and RSF-18-11-00-297. The work of D.K. was partly supported by the Grant NSF DMS-1902226. N.R. and D.K. are grateful for the hospitality at ITS ETH where he was visiting when the work was completed. N.R. would like to thank A. Borodin, I. Corwin and A. Pronko for helpful discussions on various aspects of the six vertex model.
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Keating, D., Reshetikhin, N. & Sridhar, A. Integrability of Limit Shapes of the Inhomogeneous Six Vertex Model. Commun. Math. Phys. 391, 1181–1207 (2022). https://doi.org/10.1007/s00220-022-04334-9
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DOI: https://doi.org/10.1007/s00220-022-04334-9