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Physical review. B, Condensed matter

Simulation of solitons in an Ising-like S=(1/2 antiferromagnet on a linear chain

Fumitaka Matsubara, Sakari Inawashiro

Published Feb 1, 1990• 9 citations
Publisher

Abstract

The dynamics of quantum solitons in an Ising-like S=(1/2 antiferromagnet on finite linear chains with spins N (\ensuremath{\le}15) is studied by integrating the Schr\"odinger equation of motion. Space-time correlation functions ${S}^{\mathrm{zz}}$(r,t) and their Fourier transforms, i.e., dynamical structure factor ${S}^{\mathrm{zz}}$(q,\ensuremath{\omega}), are calculated for both even and odd N. A slow but large oscillation of ${S}^{\mathrm{zz}}$(r,t) is seen, which gives a direct evidence of the occurrence of propagating domain walls, i.e., solitons. The oscillation leads to a low-energy component of ${S}^{\mathrm{zz}}$(q,\ensuremath{\omega}) whose line shape greatly depends on whether N is even or odd and on the temperature. We analyze in detail the dependence of soliton number in the line shape and give a plausible conjecture that ${S}^{\mathrm{zz}}$(q,\ensuremath{\omega}) for N=\ensuremath{\infty} should exhibit a very broad double maximum at low temperatures. We estimate ${S}^{\mathrm{zz}}$(q,\ensuremath{\omega}) at various temperatures. Our results reproduce experimental observations of ${S}^{\mathrm{zz}}$(q,\ensuremath{\omega}) on ${\mathrm{CsCoCl}}_{3}$ and ${\mathrm{CsCoBr}}_{3}$ very well over a wide temperature range.

DOI
10.1103/physrevb.41.2284

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arXiv:cond-mat/9801070•Journal of the Physical Society of Japan•Apr 15, 1998•0 citations
The dynamics of quantum solitons in an Ising-like S=(1/2 antiferromagnet on finite linear chains with spins N (\ensuremath{\le}15) is studied by integrating the Schr"odinger equation of motion. Space-time correlation functions Szz{S}^{\mathrm{zz}}Szz(r,t) and their Fourier transforms, i.e., dynamical structure factor Szz{S}^{\mathrm{zz}}Szz(q,\ensuremath{\omega}), are calculated for both even and odd N. A slow but large oscillation of Szz{S}^{\mathrm{zz}}Szz(r,t) is seen, which gives a direct evidence of the occurrence of propagating domain walls, i.e., solitons. The oscillation leads to a low-energy component of Szz{S}^{\mathrm{zz}}Szz(q,\ensuremath{\omega}) whose line shape greatly depends on whether N is even or odd and on the temperature. We analyze in detail the dependence of soliton number in the line shape and give a plausible conjecture that Szz{S}^{\mathrm{zz}}Szz(q,\ensuremath{\omega}) for N=\ensuremath{\infty} should exhibit a very broad double maximum at low temperatures. We estimate Szz{S}^{\mathrm{zz}}Szz(q,\ensuremath{\omega}) at various temperatures. Our results reproduce experimental observations of Szz{S}^{\mathrm{zz}}Szz(q,\ensuremath{\omega}) on CsCoCl3{\mathrm{CsCoCl}}_{3}CsCoCl3​ and CsCoBr3{\mathrm{CsCoBr}}_{3}CsCoBr3​ very well over a wide temperature range.
The spin dynamics of an Ising-like S =1/2 antiferromagnet with a weak next-nearest-neighbor interaction on a linear chain is studied by a perturbation method. Bound states of two domain walls, i.e., 2-soliton bound states, are found in addition to soliton-pair states. When the next-nearest-neighbor interaction is ferromagnetic, the dynamical structure factor S x x ( k , ω) exhibits a sharp peak at a lower energy and a tail at higher energies. Our results are in good agreement with experimental observations of S x x ( k , ω) on CsCoCl 3 and CsCoBr 3 at low temperatures.
Dynamics of one-dimensional Ising-like (strongly anisotropic) antiferromagnets is studied by the perturbation theory from the pure Ising limit and by an exact calculation for finite chains. Both calculations show that the des Cloizeaux-Gaudin (dC-G) “spin-wave” spectrum corresponds neither to a lower bound of excitation continuum nor to the peak position of the transverse response Sxx(Q, ω). A new interpretation is given of the spin-wave spectrum of CsCoCl3 without relying on the dC-G theory. It is also shown that at elevated temperatures Sxx(Q, ω) has a three-peak structure. The longitudinal response Sxx(Q, ω) at low temperatures has a weak peak at the position of spin wave peak, while with increasing temperature Sxx(Q, ω) is dominated by the central peak due to thermally activated solitons, which was predicted by Villain.
We consider the one-dimensional Ising-like fully anisotropic S = 1/2 Heisenberg antiferromagnetic Hamiltonian and study the dynamics of domain wall excitations in the presence of a transverse magnetic field h x . We obtain dynamical spin correlation functions along the magnetic field, S xx ( q ,ω), and perpendicular to it, S yy ( q ,ω). It is shown that the line shapes of S xx ( q ,ω) and S yy ( q ,ω) are purely symmetric at the zone boundary. It is observed in S yy ( q ,ω) for π/2< q <π that the spectral weight moves toward the low-energy side with the increase of h x . This model is applicable to the study of the spin dynamics of CsCoCl 3 in the presence of weak interchain interactions.
The effect of the transverse magnetic field h x on the spin dynamics of a one dimensional Ising-like S =1/2 antiferromagnet is discussed. Based on a picture of the propagating domain walls, we obtain dynamical spin correlation functions along the magnetic field S x x ( k ,ω) and perpendicular to it S y y ( k ,ω). A remarkable effect is seen in S y y ( k ,ω) for π/2 ≤ k ≤π, where the spectral weight moves toward the low energy side with the increase of h x . The theory is applied to the analysis of the spin dynamics of CsCoCl 3 , taking into account weak interchain interactions. Zeeman ladders occur and S y y ( k , ω) for k ∼π exhibits a novel feature under the existence of h x .
The dynamical properties of the S=1/2 antiferromagnetic XXZ chain are studied by the exact diagonalization and the recursion method of finite systems up to 24 sites. Two types of the exchange interaction are considered: one is the nearest-neighbor type, and the other is the inverse-square one. As the Ising anisotropy becomes larger, there appears a noticeable difference in the transverse component S^{xx}(q,ω) between the two types of the exchange. For the nearest-neighbor type, the peak frequency of S^{xx}(q,ω) for each q approaches the center of the continuum spectrum. On the contrary, the peak frequency for the inverse-square type moves to the upper edge of the continuum, and separates from the continuum for the anisotropy larger than the threshold value. Whether the interaction between domain walls (solitons) is absent or repulsive in the Ising limit leads to this difference in the behavior of S^{xx}(q,ω). In the longitudinal component S^{zz}(q,ω), on the other hand, the feature of the dynamics is scarcely different between the two types. The energy gap and the static properties are also discussed.