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Conference on Multimedia Modeling

Spectral weight of low-lying excitations in the one-dimensional spin 1/2 Heisenberg antiferromagnet

J. C. Bonner, Bill Sutherland, Peter M. Richards

Published Jan 1, 1974• 0 citations
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The spectral weight of low-lying excitations in the one-dimensional spin 1/2 Heisenberg antiferromagnet

J. C. Bonner, Bill Sutherland, Peter M. Richards

We have examined numerical calculations on a spin 1/2 one‐dimensional (1D) Heisenberg antiferromagnet for N=8 spins, both for the states and their spectral weights. This work is of interest because of the recent neutron scattering experiments in CuCl2⋅2NC5D5 which show the spectral weight to be concentrated at the des Cloizeaux and Pearson (dCP) spin wave frequencies. The states form a two‐parameter continuum between the dCp value E1(k) =π‖J‖ ‖sin k‖ and the upper limit E2(k) =2π‖J‖ ‖ sin(k/2) ‖. Though most of the spectral weight is at the dCP frequency for N=8, about 10% of it is found near E2 for k=π. There is no numerical evidence for the existence of singlet bound states as predicted by Ovchinnikov.

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Physical review. B, Condensed matter•Jan 1, 1986•412 citations
We have examined numerical calculations on a spin 1/2 one‐dimensional (1D) Heisenberg antiferromagnet for N=8 spins, both for the states and their spectral weights. This work is of interest because of the recent neutron scattering experiments in CuCl2⋅2NC5D5 which show the spectral weight to be concentrated at the des Cloizeaux and Pearson (dCP) spin wave frequencies. The states form a two‐parameter continuum between the dCp value E1(k) =π‖J‖ ‖sin k‖ and the upper limit E2(k) =2π‖J‖ ‖ sin(k/2) ‖. Though most of the spectral weight is at the dCP frequency for N=8, about 10% of it is found near E2 for k=π. There is no numerical evidence for the existence of singlet bound states as predicted by Ovchinnikov.
We investigate the properties of low-lying photoexcited states of a one-dimensional (1D) ionic extended Hubbard model at half-filling. Numerical analysis by using the full and Lanczos diagonalization methods shows that, in the ionic phase, there exist low-lying photoexcited states below the charge transfer gap. As a result of comparison with numerical data for the 1D antiferromagnetic (AF) Heisenberg model, it was found that, for a small alternating potential Δ, these low-lying photoexcited states are spin excitations, which is consistent with a previous analytical study [Katsura et al., Phys. Rev. Lett. 103, 177402 (2009)]. As Δ increases, the spectral intensity of the 1D ionic extended Hubbard model rapidly deviates from that of the 1D AF Heisenberg model and it is clarified that this deviation is due to the neutral-ionic domain wall, an elementary excitation near the neutral-ionic transition point.