Mass ratio of elementary excitations in frustrated antiferromagnetic chains with dimerization

Physics – Condensed Matter – Strongly Correlated Electrons

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6 pages, 4 figures

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Excitation spectra of $S=1/2$ and S=1 frustrated Heisenberg antiferromagnetic chains with bond alternation (explicit dimerization) are studied, by a combination of analytical and numerical methods. The system undergoes a dimerization transition at a critical bond alternation parameter $\delta=\delta_{\rm c}$, where $\delta_{\rm c} = 0$ for the $S=1/2$ chain. Except at the transition, the SU(2) symmetric sine-Gordon theory is known to be an effective field theory of the system. The sine-Gordon theory has a SU(2)- triplet and a SU(2) singlet of elementary excitation, and the mass ratio $r$ of the singlet to the triplet is $\sqrt{3}$. However, our numerical calculation with the infinite time-evolving block decimation method shows that $r$ depends on the frustration (next-nearest neighbor coupling) and is generally different from $\sqrt{3}$. This can be understood as an effect of marginal perturbation to the sine-Gordon theory. In fact, at the critical frustration separating the second-order and first-order dimerization transitions, the marginal operator vanishes and $r=\sqrt{3}$ holds. We derive the mass ratio $r$ analytically using form-factor perturbation theory combined with a renormalization-group analysis. Our formula agrees well with the numerical results, confirming the theoretical picture. The present theory also implies that, in the very vicinity of the second-order dimerization critical point, the mass ratio approaches to $\sqrt{3}$. However, such region is extremely small and would be difficult to observe numerically.

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