Date of Original Version
The conformal anomaly c determines the universality class of a model system in statistical mechanics. The value of c characterizes both 2D classical models and their 1D quantum counterparts. The conformal anomaly may therefore be determined numerically for quantum spin chains using the relation: E 0(N)≂E 0(∞)−(NΔE/12)c(1/N 2), where E 0 (N) is the ground‐state energy of an N‐spin finite system, E 0 (∞) is the ground‐state energy in the thermodynamic limit, and ΔE is the energy gap between the ground state at k=0 and the first excited state of the dispersion curve at k=2π/N. The numerical approach is highly successful when tested on the integrable s= 1/2 Heisenberg antiferromagnetic X X Z chain and the integrable s=1 SU(2) model. The method gives c=1 to within 2% accuracy for the s=1 and (3)/(2) X Y chains, placing them in the universality class of the 2D X Y model. The result c=1 (2% accuracy) is obtained for the s= (3)/(2) Heisenberg antiferromagnetic chain, in agreement with the Haldane prediction. The s=1 pure antiferromagnetic biquadratic chain and the s=1 X X Z model with uniaxial anisotropy in the vicinity of the critical point Δ=Δ2 ∼1.15 −1.18 have also been studied.
Jill C. Bonner and John B. Parkinson. Quantum spin chains and the conformal anomaly. J. Appl. Phys. 63 (1988), 3543-3545.
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The following article appeared in Journal of Applied Physics and may be found at http://dx.doi.org/10.1063/1.340737.