We explicitly describe certain components of the finite size groundstate of the inhomogeneous transfer matrix of the O(n = 1) loop model on a strip with nontrivial boundaries on both sides. In addition we compute explicitly the groundstate normalisation which is given as a product of four symplectic characters.

Employing an inhomogeneous solvable lattice model, we derive an exact expression for a boundary-to-boundary edge current on a lattice of finite width. This current is an example of a class of parafermionic observables recently introduced in an attempt to rigorously prove conformal invariance of the scaling limit of critical two-dimensional lattice models. It also corresponds to the spin current at the spin-Quantum Hall transition in a model introduced by Chalker and Coddington, and generalized by Gruzberg, Ludwig and Read. Our result is derived from a solution of the $q$-deformed Knizhnik-Zamolodchikov equation, and is expressed in terms of a symplectic Toda-lattice wave-function.Comment: 22 pages, 26 postscript figures, revised versio

We obtain an exact finite-size expression for the probability that a percolation hull will touch the boundary, on a strip of finite width. Our calculation is based on the q-deformed Knizhnik-Zamolodchikov approach, and the results are expressed in terms of symplectic characters. In the large size limit, we recover the scaling behaviour predicted by Schramm's left-passage formula. We also derive a general relation between the left-passage probability in the Fortuin-Kasteleyn cluster model and the magnetisation profile in the open XXZ chain with diagonal, complex boundary terms. * Yacine.Ikhlef@unige.ch † Anita.Ponsaing@unige.ch arXiv:1202.5476v1 [math-ph]

We compute the boundary entropy for bond percolation on the square lattice in the presence of a boundary loop weight, and prove explicit and exact expressions on a strip and on a cylinder of size L. For the cylinder we provide a rigorous asymptotic analysis which allows for the computation of finitesize corrections to arbitrary order. For the strip we provide exact expressions that have been verified using high-precision numerical analysis. Our rigorous and exact results corroborate an argument based on conformal field theory, in particular concerning universal logarithmic corrections for the case of the strip due to the presence of corners in the geometry. We furthermore observe a crossover at a special value of the boundary loop weight.

We study the induced spherical ensemble of non-Hermitian matrices with real quaternion entries (considering each quaternion as a 2 × 2 complex matrix). We define the ensemble by the matrix probability distribution function that is proportional toThese matrices can also be constructed via a procedure called 'inducing', using a product of a Wishart matrix (with parameters n, N ) and a rectangular Ginibre matrix of size (N +L)×N . The inducing procedure imposes a repulsion of eigenvalues from 0 and ∞ in the complex plane, with the effect that in the limit of large matrix dimension, they lie in an annulus whose inner and outer radii depend on the relative size of L, n and N . By using functional differentiation of a generalized partition function, we make use of skew-orthogonal polynomials to find expressions for the eigenvalue m-point correlation functions, and in particular the eigenvalue density (given by m = 1).We find the scaled limits of the density in the bulk (away from the real line) as well as near the inner and outer annular radii, in the four regimes corresponding to large or small values of n and L. After a stereographic projection the density is uniform on a spherical annulus, except for a depletion of eigenvalues on a great circle corresponding to the real axis (as expected for a real quaternion ensemble). We also form a conjecture for the behaviour of the density near the real line based on analogous results in the β = 1 and β = 2 ensembles; we support our conjecture with data from Monte Carlo simulations of a large number of matrices drawn from the β = 4 induced spherical ensemble.