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arXiv:2512.24182 · SciPost Physics

Tensor-network analysis of root patterns in the XXX model with open boundaries

Zhouzheng Ji, Pei Sun, Xiaotian Xu, Yi Qiao, Junpeng Cao, Wen‐Li Yang

Published Sep 3, 2026• 0 citations
arXivHTMLPDF

Abstract

The string hypothesis of Bethe roots is a cornerstone in the thermodynamic analysis of quantum integrable systems, since it connects root configurations with physical quantities such as the ground-state energy, surface energy and excitation spectra. For integrable models with U(1) U ( 1 ) symmetry, this connection is well established. When the U(1) U ( 1 ) symmetry is broken by generic non-diagonal boundary fields, however, the off-diagonal Bethe Ansatz leads to an inhomogeneous T\text{--}Q T – Q relation whose Bethe roots have highly nontrivial distributions. This raises two fundamental questions: whether the zero roots and the ODBA Bethe roots still possess regular and classifiable structures in the large-size limit, and whether such structures can be used to extract physical quantities. In this work, we address these two questions for the isotropic Heisenberg spin chain with non-diagonal open boundaries. By combining tensor-network algorithms with Bethe-Ansatz techniques, we determine the zero-root and Bethe-root configurations associated with the \Lambda\text{--}\theta Λ – θ relation and the inhomogeneous Bethe Ansatz equations for large system sizes, up to N\simeq 60 N ≃ 60 and 100 100 . We find that, despite the absence of U(1) U ( 1 ) symmetry, the roots exhibit well-organized patterns. The zero roots form bulk strings, boundary strings, additional roots, and a helical half-spinon, while the ODBA Bethe roots split into four geometric classes: regular roots, line roots, arc roots and paired-line roots. We further show that these root structures are not merely numerical patterns, but contain direct thermodynamic information. In particular, the geometric structure of the ODBA Bethe roots allows us to derive analytic expressions for the surface energy and elementary excitation energies. This demonstrates that the full ODBA Bethe-root configuration can serve as a thermodynamically meaningful object in a U(1) U ( 1 ) -symmetry-broken open spin chain. A comparison with the t\text{--}W t – W scheme shows that the zero-root description has a simpler topology, while the ODBA Bethe roots provide a direct route to physical quantities. Our results therefore provide a framework for studying root structures and thermodynamic properties in quantum integrable models without U(1) U ( 1 ) symmetry.

DOI
10.21468/scipostphys.21.3.051

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The string hypothesis of Bethe roots is a cornerstone in the thermodynamic analysis of quantum integrable systems, since it connects root configurations with physical quantities such as the ground-state energy, surface energy and excitation spectra. For integrable models with U(1) U ( 1 ) symmetry, this connection is well established. When the U(1) U ( 1 ) symmetry is broken by generic non-diagonal boundary fields, however, the off-diagonal Bethe Ansatz leads to an inhomogeneous T\text{--}Q T – Q relation whose Bethe roots have highly nontrivial distributions. This raises two fundamental questions: whether the zero roots and the ODBA Bethe roots still possess regular and classifiable structures in the large-size limit, and whether such structures can be used to extract physical quantities. In this work, we address these two questions for the isotropic Heisenberg spin chain with non-diagonal open boundaries. By combining tensor-network algorithms with Bethe-Ansatz techniques, we determine the zero-root and Bethe-root configurations associated with the \Lambda\text{--}\theta Λ – θ relation and the inhomogeneous Bethe Ansatz equations for large system sizes, up to N\simeq 60 N ≃ 60 and 100 100 . We find that, despite the absence of U(1) U ( 1 ) symmetry, the roots exhibit well-organized patterns. The zero roots form bulk strings, boundary strings, additional roots, and a helical half-spinon, while the ODBA Bethe roots split into four geometric classes: regular roots, line roots, arc roots and paired-line roots. We further show that these root structures are not merely numerical patterns, but contain direct thermodynamic information. In particular, the geometric structure of the ODBA Bethe roots allows us to derive analytic expressions for the surface energy and elementary excitation energies. This demonstrates that the full ODBA Bethe-root configuration can serve as a thermodynamically meaningful object in a U(1) U ( 1 ) -symmetry-broken open spin chain. A comparison with the t\text{--}W t – W scheme shows that the zero-root description has a simpler topology, while the ODBA Bethe roots provide a direct route to physical quantities. Our results therefore provide a framework for studying root structures and thermodynamic properties in quantum integrable models without U(1) U ( 1 ) symmetry.
Abstract Finding out root patterns of quantum integrable models is an important step to study their physical properties in the thermodynamic limit. Especially for models without U(1) symmetry, their spectra are usually given by inhomogeneous T − Q relations and the Bethe root patterns are still unclear. In this paper with the antiperiodic XXZ spin chain as an example, an analytic method to derive both the Bethe root patterns and the transfer-matrix root patterns in the thermodynamic limit is proposed. Based on them the ground state energy and elementary excitations in the gapped regime are derived. The present method provides an universal procedure to compute physical properties of quantum integrable models in the thermodynamic limit.
The XXX spin- \frac{1}{2} 1 2 Heisenberg chain with non-diagonal boundary fields represents a cornerstone model in the study of integrable systems with open boundaries. Despite its significance, solving this model exactly has remained a formidable challenge due to the breaking of U(1) U ( 1 ) symmetry. Building on the off-diagonal Bethe Ansatz (ODBA), we derive a set of nonlinear integral equations (NLIEs) that encapsulate the exact spectrum of the model. For U(1) U ( 1 ) symmetric spin- \frac{1}{2} 1 2 chains such NLIEs involve two functions a(x) a ( x ) and \bar{a}(x) a ‾ ( x ) coupled by an integration kernel with short-ranged elements. The solution functions show characteristic features for arguments at some length scale which grows logarithmically with system size N N . In the case considered here the U(1) U ( 1 ) symmetry is broken by the non-diagonal boundary fields and the equations involve a novel third function c(x) c ( x ) , which captures the inhomogeneous contributions to the T T - Q Q relation in the ODBA. The kernel elements coupling this function to the standard ones are long-ranged and lead for the ground-state to a winding phenomenon. In \log(1+a(x)) log ( 1 + a ( x ) ) and \log(1+\bar a(x)) log ( 1 + a ‾ ( x ) )
We study the exact solution of the Gaudin model with Dzyaloshinsky–Moriya and Kaplan–Shekhtman–Entin–Wohlman–Aharony interactions. The energy and Bethe ansatz equations of the Gaudin model can be obtained via the off-diagonal Bethe ansatz method. Based on the off-diagonal Bethe ansatz solutions, we construct the Bethe states of the inhomogeneous XXX Heisenberg spin chain with the generic open boundaries. By taking a quasi-classical limit, we give explicit closed-form expression of the Bethe states of the Gaudin model. From the numerical simulations for the small-size system, it is shown that some Bethe roots go to infinity when the Gaudin model recovers the U(1) symmetry. Furthermore, it is found that the contribution of those Bethe roots to the Bethe states is a nonzero constant. This fact enables us to recover the Bethe states of the Gaudin model with the U(1) symmetry. These results provide a basis for the further study of the thermodynamic limit, correlation functions, and quantum dynamics of the Gaudin model.
This chapter addresses the long-standing challenge of constructing the Bethe wave function in large but finite volumes via the diagonalization of the transfer matrix within the spin representation. While the coordinate Bethe ansatz provides effective tools for specific models, it becomes increasingly cumbersome in systems with internal degrees of freedom, such as the Lieb–Liniger model. The algebraic Bethe ansatz offers a more general and systematic framework, particularly well suited for handling nested structures. Spin chains serve as a natural setting for this formalism, offering both mathematical richness and physical relevance as models of interacting quantum spins. Starting from the Heisenberg spin chain, the chapter introduces the algebraic structure underpinning the method, including the R -matrix formulation, quantum group symmetries, and the construction of the transfer matrix. To connect the algebraic formalism with thermodynamic behavior, the chapter explores the string hypothesis, which organizes solutions to the Bethe equations into regular complex patterns. This leads naturally to the Bethe–Takahashi equations, which govern the thermodynamic limit of integrable spin chains. These tools enable a tractable analysis of excited states and physical observables, establishing a foundation for applying the algebraic Bethe ansatz to a broader class of quantum integrable systems.
Recently, the XXX spin chain with arbitrary boundary fields was successfully solved [1] via the off-diagonal Bethe ansatz method [2]. The correctness and the completeness of this solution were numerically verified by Nepomechie for one choice of the parameterizations [3]. In this paper, we discuss further the completeness of another parameterization of the Bethe ansatz equations and its reduction to the parallel boundary field case. The numerical results show that when the relative angle between the boundary fields turns to zero, both the T-Q relations and the Bethe ansatz equations are reduced to the ones obtained by the conventional Bethe ansatz methods. This allows us to establish a one-to-one correspondence between the Bethe roots of the unparallel boundary field case and those of the parallel boundary field case. In the thermodynamic limit, those two sets of Bethe roots tend to the same and the contribution of the relative angle to the energy is in the order of 1/N.