2017
DOI: 10.1007/978-3-319-48487-7
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An Introduction to Integrable Techniques for One-Dimensional Quantum Systems

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Cited by 223 publications
(253 citation statements)
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References 143 publications
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“…Working directly in the limit L → ∞, this is a well-known problem in terms of the thermodynamic Bethe Ansatz (TBA) [46,47]. Indeed, the eigenstates of the XXZ chain are parametrized by rapidities λ, corresponding to magnon excitations created upon the fully polarized state.…”
Section: Magnetization Profilesmentioning
confidence: 99%
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“…Working directly in the limit L → ∞, this is a well-known problem in terms of the thermodynamic Bethe Ansatz (TBA) [46,47]. Indeed, the eigenstates of the XXZ chain are parametrized by rapidities λ, corresponding to magnon excitations created upon the fully polarized state.…”
Section: Magnetization Profilesmentioning
confidence: 99%
“…In particular, the ground state has a simple Fermi sea character, with real rapidities fully occupying an interval λ ∈ [−Λ, Λ]. While for finite L the rapidities satisfy some appropriate quantization conditions, in the thermodynamic limit the roots become continuous, and their density ρ(λ) follows from the TBA equation [46,47] …”
Section: Magnetization Profilesmentioning
confidence: 99%
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“…The effect of frustration induced by the boundary conditions has been already considered in integrable systems with a continuous U(1) symmetry at vanishing external field as the XXZ chain obtained by setting γ=0 and h=0 in (1) [21][22][23][24], where the eigenstates can be constructed in terms of individual excitations. Thus, while for even lengths N=2M the ground-state can achieve zero total magnetization S 0 T Z = and be characterized as a spinon vacuum [25], in the frustrated case N=2M+1 there are two equivalent ground-states with S T Z 1 2 =  (whose degeneracy is immediately lifted for a nonzero h), which can be interpreted as due to the presence of a traveling single spinon excitation. The goal of the present paper is to analyze the case of systems with discrete global symmetries 2  , which, thus, do not conserve particle number.…”
Section: Introductionmentioning
confidence: 99%
“…, 1 where the two-body interaction between the particles is described by a zero-range delta-function potential of strength g [44]. While exact solutions for this Hamiltonian exist in the absence of an external potential [45,46], only limiting cases can be solved in other situations. One regime in which the Hamiltonian (1) can be solved exactly is the strongly interacting TG limit.…”
Section: Basic Modelmentioning
confidence: 99%