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Physica A Statistical Mechanics and its Applications

Effective critical exponents in two-dimensional systems from conformal field theory

P. Zhou

Published Jun 1, 1991• 0 citations
Publisher
DOI
10.1016/0378-4371(91)90335-a

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Introduction The long distance asymptotics of correlation functions in integrable models have attracted long-standing interest. For the gapless one-dimensional systems considered in this book, zero temperature is a critical point. At zero temperature, ( T = 0), correlation functions decay as a power of the distance, but for T > 0, correlation functions decay exponentially. The powers of the distance by which correlation functions decay at zero temperature are called the critical exponents and they are the subject of this chapter. A recent development in the understanding of critical phenomena in (1+1)-dimensional systems is connected with conformal field theory which provides a powerful method for calculating critical exponents. However, many important results in (1+1)-dimensional systems have been obtained from perturbation calculations and renormalization group treatments, and. It should also be noted that the quantum inverse scattering method (QISM) approach to correlation functions confirms the predictions of conformal field theory (CFT), but more importantly QISM techniques show that the critical exponents of integrable models depend only on the underlying R-matrix. The Luttinger liquid approach is very powerful; it is also close to CFT. This approach is essentially based on the representation of a critical one-dimensional model in terms of a gaussian model. In the framework of this approach, the critical exponent was calculated first for Bethe Ansatz solvable models with a single degree of freedom. One should also mention the bosonization technique.
The one dimensional S=1/2S=1/2S=1/2 Heisenberg model with dimerization (1−j1-j1−j) and quadrumerization (δδδ) in the magnetic field is studied by means of the numerical exact diagonalization of finite size systems and the conformal field theory. It is found that the magnetization plateau at half of the saturation value exists for δ≠0δ\neq 0δ=0. For δ=0δ= 0δ=0, this model is described by the conformal field theory with central charge c=1c=1c=1 at this value of magnetization. The critical exponent ννν which characterizes the δδδ-dependence of the width of the plateau is calculated using the level spectroscopy method. The jjj-dependence of the critical exponent ννν is found to be non-monotonic and discontinuous at j=0j = 0j=0. The effective theory of the magnetization plateau is also presented for various limiting cases.