The cubic lattice gas, a generalization of the
n-component face-cubic model, is studied in two dimensions by variational renormalization-group techniques for general
n, and by an exact mapping onto a solid-on-solid model for
n=2. This approach reveals new interconnections among the class of cubic, Potts, and Ashkin-Teller phase-transition phenomena. In particular, it is shown that the fixed line of the Ashkin-Teller lattice gas serves as the backbone for a hierarchy of pairs of fixed points which branch off from it, as
n is decreased from 2, at special points where two operators are marginal. The phase diagrams of the pure and dilute
n-component cubic models are obtained and the orders of all transitions are determined. The cubic phase transition is found to be first order for all
n>nc=2. The evolution of the results as a function of dimensionality is discussed briefly.
We investigate the boundary critical phenomena of the one-dimensional quantum Ashkin-Teller model using boundary conformal field theory and density matrix renormalization group (DMRG) simulations. Based on the
Z2-orbifold of the
c=1 compactified boson boundary conformal field theory, we construct microscopic lattice boundary terms that renormalize to the stable conformal boundary conditions, utilizing simple current extensions and the underlying
SU(2) symmetry to explicitly characterize the four-state Potts point. We validate these theoretical identifications via finite-size spectroscopy of the lattice energy spectra, confirming their consistency with
D4 symmetry and Kramers-Wannier duality. Finally, we discuss the boundary renormalization group flows among these identified fixed points to propose a global phase diagram for the boundary criticality.
A real-space rescaling technique (decimation) is used to study the critical properties of the bond-dilute, S state Ashkin-Teller-Potts model on the square lattice. Fixed points and critical exponents are obtained and critical curves plotted for values of S from 1 to 4. For S=1, 2 the dilute model exhibits the same critical behaviour as the pure system. However, for S=3, 4, there is crossover to a new dilute fixed point. The transition remains second order but exhibits new values of the critical exponents. This behaviour is in accord with the Harris criterion (1974).