Abstract

Recently there has been a renewed interest in the spectra and role in dynamical properties of excited states of the spin-1/2 Heisenberg antiferromagnetic chain in longitudinal magnetic fields associated with Bethe strings. The latter are bound states of elementary magnetic excitations described by Bethe-ansatz complex non-real rapidities. Previous studies on this problem referred to finite-size systems. Here we consider the thermodynamic limit and study it for the isotropic spin-1/2 Heisenberg XXX chain in a longitudinal magnetic field. We confirm that also in that limit the most significant spectral weight contribution from Bethe strings leads to (k,ω)-plane gapped continua in the spectra of the spin dynamical structure factors S+−(k,ω) and Sxx(k,ω)=Syy(k,ω). The contribution of Bethe strings to Szz(k,ω) is found to be small at low spin densities m and to become negligible upon increasing that density above m≈0.317. For S−+(k,ω), that contribution is found to be negligible at finite magnetic field. We derive analytical expressions for the line shapes of S+−(k,ω), Sxx(k,ω)=Syy(k,ω), and Szz(k,ω) valid in the (k,ω)-plane vicinity of singularities located at and just above the gapped lower thresholds of the Bethe-string states's spectra. As a side result and in order to provide an overall physical picture that includes the relative (k,ω)-plane location of all spectra with a significant amount of spectral weight, we revisit the general problem of the line-shape of the transverse and longitudinal spin dynamical structure factors at finite magnetic field and excitation energies in the (k,ω)-plane vicinity of other singularities. This includes those located at and just above the lower thresholds of the spectra that stem from excited states described by only real Bethe-ansatz rapidities.

Highlights

  • There has been a renewed interest in bound states of elementary magnetic excitations named Bethe strings known long ago [1,2,3,4,5]

  • In spite of Bethe strings being a rather theoretical issue, as they were first found and identified within the Bethe ansatz solution of spin and electronic integrable models in some classes of energy eigenstates described by complex non-real spin rapidities [1,2], this renewed interest is due, in part, to their experimental identification and realization in spin-chain compounds whose magnetic properties are described by the spin-1/2 Heisenberg chain in longitudinal magnetic fields [6,7,8,9,10]

  • Most previous studies on the spin dynamical properties of the spin-1/2 XXX chain in a longitudinal magnetic field focused on the contribution from energy eigenstates described by real Betheansatz rapidities, which are associated with most spectral weight of the spin dynamical structure factors

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Summary

Introduction

There has been a renewed interest in bound states of elementary magnetic excitations named Bethe strings known long ago [1,2,3,4,5]. Most previous studies on the spin dynamical properties of the spin-1/2 XXX chain in a longitudinal magnetic field focused on the contribution from energy eigenstates described by real Betheansatz rapidities, which are associated with most spectral weight of the spin dynamical structure factors. Several such studies considered finite-size systems and relied on different methods. And as a side result, in order to provide an overall physical picture that includes the relative (k, ω)-plane location of all features with a significant amount of spectral weight, we account for the contributions from all types of states that lead to gapped and gapless lower threshold singularities in the spin dynamical structure factors. Two Appendices provide useful side information needed for the studies of this paper

The model and the spin dynamical structure factors
The spectral functionals of the extended dynamical theory
The present quantum problem extended subspace
General expressions of the extended dynamical theory’s spectral functionals
Constrains to the momentum dependent exponents’ k intervals
Dynamical structure factors’s spectra
The line shape near the singularities of the dynamical structure factors
Limiting behaviors of the spin dynamical structure factors
Discussion and concluding remarks
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