Starting with the Ising model, statistical models with global symmetries provide fruitful approaches to interesting physical systems, for example percolation or polymers. These include the O(n)O(n) model (symmetry group O(n)O(n)) and the Potts model (symmetry group S_QSQ). Both models make sense for n,Q∈ \mathbb{C}n,Q∈ℂ and not just n,Q∈ \mathbb{N}n,Q∈ℕ, and both give rise to a conformal field theory in the critical limit. Here, we study similar models based on the group PSU(n)PSU(n). We focus on the two-dimensional case, where the models can be described either as gases of non-intersecting orientable loops, or as alternating spin chains. This allows us to determine their spectra either by computing a twisted torus partition function, or by studying representations of the walled Brauer algebra. In the critical limit, our models give rise to a CFT that exists for any n∈\mathbb{C}n∈ℂ and has a global PSU(n)PSU(n) symmetry. Its spectrum is similar to those of the O(n)O(n) and Potts CFTs, but a bit simpler. We conjecture that the O(n)O(n) CFT is a \mathbb{Z}_2ℤ2 orbifold of the PSU(n)PSU(n) CFT, where \mathbb{Z}_2ℤ2 acts as complex conjugation.
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