Delta-Function Bose Gas Picture of S=1 Antiferromagnetic Quantum Spin Chains Near Critical Fields

TL;DR

This paper investigates the validity of the delta-function Bose gas model for describing the magnetization behavior of S=1 antiferromagnetic chains near critical magnetic fields, revealing distinct regimes and critical behaviors.

Contribution

It demonstrates the applicability of the delta-function Bose gas picture near critical fields and identifies a critical value of the biquadratic interaction parameter separating different magnetic behaviors.

Findings

Excellent agreement between Bose gas model and PWFRG calculations near saturation field.

Identification of a critical biquadratic parameter $eta_c \\approx 0.41$ separating different critical behaviors.

Transition from square-root to 1/4 power law in magnetization near $H_c$ as $eta$ approaches $eta_c$.

Abstract

We study the zero-temperature magnetization curve (M-H curve) of the S=1 bilinear-biquadratic spin chain, whose Hamiltonian is given by $H=\sum_{i} S_i S_{i+1}+\beta (S_iS_{i+1})^2 with $0 \leq \beta <1$. We focus on validity of the delta-function bose-gas picture near the two critical fields: the saturation field $H_s$ and the lower critical field $H_c$ associated with the Haldane gap. Near $H_s$, we take ``low-energy effective S-matrix'' approach, which gives correct effective bose-gas coupling constant $c$, different from the spin-wave value. Comparing the M-H curve of the bose gas with the product-wavefunction renormalization group (PWFRG) calculation, excellent agreement is seen. Near $H_c$, comparing the PWFRG result with the bose-gas prediction, we find that there are two distinct regions of $\beta$ separated by a critical value $\beta_c(\approx 0.41)$. In the region $0<\beta<\beta_c$, the effective coupling $c$ is positive but rather small. The small value of $c$ makes the ``critical region'' of the square-root behavior $M\sim \sqrt{H-H_c}$ very narrow. Further, we find that in the $\beta \to \beta_c-0$, the square-root behavior transmutes to a different one, $M\sim (H-H_c)^{1/4}$. In the region $\beta_c<\beta <1$, the square-root behavior is rather distinct, but the effective coupling $c$ becomes negative.