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Modern Physics Letters B

EXACT n-SPINON DYNAMIC STRUCTURE FACTOR OF THE HEISENBERG MODEL

A. Hamid Bougourzi

Published Oct 30, 1996• 9 citations
Publisher

Abstract

Using the spinon picture we derive an integral representation for the exact n-spinon dynamic structure factor of the spin-1/2 Heisenberg model.
DOI
10.1142/s0217984996001401

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Exact n-spinon dynamic structure factor of the Heisenberg model

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We revisit our initial derivations of the exact 2-spinon $S_2$ and 4-spinon $S_4$ dynamical structure factors (DSF). First we show that the latter derivations had normalization factors that are twice and quadriple the correct ones respectively. This means that $S_2$ contributes not 72% as was previously thought but 36% to the total DSF. We also calculated the contribution of $S_4$ to be between 18% and 20% and not 27% as was calculated by Caux and Hagemans. In fact we show that the latter reference had also the normalization factor twice the correct value and had it done the numeric integrations correctly it would have obtained a contribution between 36% and 40% for $S_4$. Furthermore, we prove that its claim that our initial derivation of $S_4$ was also incorrect in its dependency on the spectral parameters is incorrect because fixing the momentun transfer $k$ up to $2π$ as the latter reference did to justify its claim only amounts to mutltiplying the overall factor by 2 because as we will prove in this paper $S_4$ is periodic in $k$ with period $2π$. Also in this paper we derive $S_n$ for general $n$ by following a different approach compared to our initial derivation of $S_4$. Although for $S_4$ both the new derivation and the initial one lead to equivalent formulas that are expressed differently, the new form presented in this paper is much more elegant and compact and also reveals new hidden and nontrivial symmetries which substantially simplify the numeric evaluation of $S_4$ and its sum rules. Moreover based on the results of this paper we propose a simple approximation to the total DSF of the Heisenberg model. Finally we comment on how our work might resolve the discrepancy between the exact theoretic results and experiemntal data as reported by Zaliznyak et al.

arXiv:1402.3855•Feb 16, 2014•1 citation

The four-spinon dynamical structure factor of the Heisenberg chain

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We compute the exact four-spinon contribution to the zero-temperature dynamical structure factor of the spin-1/2 Heisenberg isotropic antiferromagnet in zero magnetic field, directly in the thermodynamic limit. We make use of the expressions for matrix elements of local spin operators obtained by Jimbo and Miwa using the quantum affine symmetry of the model, and of their adaptation to the isotropic case by Abada, Bougourzi and Si-Lakhal (correcting some overall factors). The four-spinon contribution to the first frequency moment sum rule at fixed momentum is calculated. This shows, as expected, that most of the remaining correlation weight above the known two-spinon part is carried by four-spinon states. Our results therefore provide an extremely accurate description of the exact structure factor.

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From Quantum Affine Groups to the Exact Dynamical Correlation Function of the Heisenberg Model

A. Hamid Bougourzi, M. Couture, M. Kacir

The exact form factors of the Heisenberg models XXX and XXZ have been recently computed through the quantum affine symmetry of XXZ model in the thermodynamic limit. We use them to derive an exact formula for the contribution of two spinons to the dynamical correlation function of XXX model at zero temperature.

arXiv:q-alg/9606010•International Journal of Modern Physics B•Jan 20, 1997•0 citations
We derive the exact contribution of two spinons to the dynamical correlation function of the spin-\textonehalf{} Heisenberg model. For this, we use the isotropic limits of the exact form factors that have been recently computed through the quantum affine symmetry of the anisotropic Heisenberg model XXZ\mathrm{XXZ}XXZ.
We revisit our initial derivations of the exact 2-spinon S2S_2S2​ and 4-spinon S4S_4S4​ dynamical structure factors (DSF). First we show that the latter derivations had normalization factors that are twice and quadriple the correct ones respectively. This means that S2S_2S2​ contributes not 72% as was previously thought but 36% to the total DSF. We also calculated the contribution of S4S_4S4​ to be between 18% and 20% and not 27% as was calculated by Caux and Hagemans. In fact we show that the latter reference had also the normalization factor twice the correct value and had it done the numeric integrations correctly it would have obtained a contribution between 36% and 40% for S4S_4S4​. Furthermore, we prove that its claim that our initial derivation of S4S_4S4​ was also incorrect in its dependency on the spectral parameters is incorrect because fixing the momentun transfer kkk up to 2π2π2π as the latter reference did to justify its claim only amounts to mutltiplying the overall factor by 2 because as we will prove in this paper S4S_4S4​ is periodic in kkk with period 2π2π2π. Also in this paper we derive SnS_nSn​ for general nnn by following a different approach compared to our initial derivation of S4S_4S4​. Although for S4S_4S4​ both the new derivation and the initial one lead to equivalent formulas that are expressed differently, the new form presented in this paper is much more elegant and compact and also reveals new hidden and nontrivial symmetries which substantially simplify the numeric evaluation of S4S_4S4​ and its sum rules. Moreover based on the results of this paper we propose a simple approximation to the total DSF of the Heisenberg model. Finally we comment on how our work might resolve the discrepancy between the exact theoretic results and experiemntal data as reported by Zaliznyak et al.
We compute the exact four-spinon contribution to the zero-temperature dynamical structure factor of the spin-1/2 Heisenberg isotropic antiferromagnet in zero magnetic field, directly in the thermodynamic limit. We make use of the expressions for matrix elements of local spin operators obtained by Jimbo and Miwa using the quantum affine symmetry of the model, and of their adaptation to the isotropic case by Abada, Bougourzi and Si-Lakhal (correcting some overall factors). The four-spinon contribution to the first frequency moment sum rule at fixed momentum is calculated. This shows, as expected, that most of the remaining correlation weight above the known two-spinon part is carried by four-spinon states. Our results therefore provide an extremely accurate description of the exact structure factor.