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arXiv:2209.14416 · Journal of High Energy Physics

On Bethe eigenvectors and higher transfer matrices for supersymmetric spin chains

Kang Lu

Published Apr 24, 2023• 2 citations
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Abstract

Abstract We study the $$ {\mathfrak{gl}}_{m\mid n} $$ gl m ∣ n XXX spin chains defined on tensor products of highest weight $$ {\mathfrak{gl}}_{m\mid n} $$ gl m ∣ n -modules. We show that the on-shell Bethe vectors are eigenvectors of higher transfer matrices and compute the corresponding eigenvalues. Then we take the classical limits and obtain the corresponding results for the $$ {\mathfrak{gl}}_{m\mid n} $$ gl m ∣ n Gaudin models.

DOI
10.1007/jhep04(2023)120

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Abstract We study the glm∣n{\mathfrak{gl}}_{m\mid n}glm∣n​ gl m ∣ n XXX spin chains defined on tensor products of highest weight glm∣n{\mathfrak{gl}}_{m\mid n}glm∣n​ gl m ∣ n -modules. We show that the on-shell Bethe vectors are eigenvectors of higher transfer matrices and compute the corresponding eigenvalues. Then we take the classical limits and obtain the corresponding results for the glm∣n{\mathfrak{gl}}_{m\mid n}glm∣n​ gl m ∣ n Gaudin models.
We implement fully the algebraic Bethe ansatz for the XXX Heisenberg spin chain in the case when both boundary matrices can be brought to the upper-triangular form. We define the Bethe vectors which yield the strikingly simple expression for the off shell action of the transfer matrix, deriving the spectrum and the relevant Bethe equations. We explore further these results by obtaining the off shell action of the generating function of the Gaudin Hamiltonians on the corresponding Bethe vectors through the so-called quasi-classical limit. Moreover, this action is as simple as it could possibly be, yielding the spectrum and the Bethe equations of the Gaudin model.
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In this paper we clarify the relationship between inhomogeneous quantum spin chains and classical integrable many-body systems. It provides an alternative (to the nested Bethe ansatz) method for computation of spectra of the spin chains. Namely, the spectrum of the quantum transfer matrix for the inhomogeneous $ gl $ n -invariant XXX spin chain on N sites with twisted boundary conditions can be found in terms of velocities of particles in the rational N -body Ruijsenaars-Schneider model. The possible values of the velocities are to be found from intersection points of two Lagrangian submanifolds in the phase space of the classical model. One of them is the Lagrangian hyperplane corresponding to fixed coordinates of all N particles and the other one is an N -dimensional Lagrangian submanifold obtained by fixing levels of N classical Hamiltonians in involution. The latter are determined by eigenvalues of the twist matrix. To support this picture, we give a direct proof that the eigenvalues of the Lax matrix for the classical Ruijsenaars-Schneider model, where velocities of particles are substituted by eigenvalues of the spin chain Hamiltonians, calculated through the Bethe equations, coincide with eigenvalues of the twist matrix, with certain multiplicities. We also prove a similar statement for the $ gl $ n Gaudin model with N marked points (on the quantum side) and the Calogero-Moser system with N particles (on the classical side). The realization of the results obtained in terms of branes and supersymmetric gauge theories is also discussed.