Is There a z-Theorem for Dynamic Critical Exponents?

Marcel den Nijs

Department of Physics, University of Washington,
Seattle, Washington 98195-1560

Proceedings of the 4th CTP Workshop on Statistical Physics
eds. D.Kim, H.Park, and B.Kahng, pages 272-292 (World Scientific, 1997).



abstract:

Dynamic processes are related to ground state properties of many-body quantum systems and also to equilibrium critical phenomena. For example, KPZ type growth of a line interface, describes also the ground state properties of interacting electrons running around a ring in the presence of an electric field, and the equilibrium crystal shape at a facet-ridge endpoint. These equivalences suggest we search for generalizations of conformal field theory to classify scaling properties of time evolution operators in D=1+1 dimensions: for Tomonaga-Luttinger liquids and conformal field theory the ``dynamic critical exponent" is equal to z=1; for non-relativistic electrons and EW type growth z=2; and for KPZ type growth z=1.5. Phase diagrams of specific models contain all four dynamic universality classes and the crossover scaling is such that z>1 typically decreases. The z-theorem explains this. The crossover from EW to KPZ type growth, and from isotropic to directed percolation are examples.

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