Abstract:The six-vertex model with domain wall boundary conditions, or square ice, is considered for particular values of its parameters, corresponding to 1-, 2-, and 3-enumerations of alternating sign matrices (ASMs). Using Hankel determinant representations for the partition function and the boundary correlator of homogeneous square ice, it is shown how the ordinary and refined enumerations can be derived in a very simple and straightforward way. The derivation is based on the standard relationship between Hankel det… Show more
Abstract. The problem of the limit shape of large alternating sign matrices (ASMs) is addressed by studying the emptiness formation probability (EFP) in the domain-wall six-vertex model. Assuming that the limit shape arises in correspondence to the 'condensation' of almost all solutions of the saddle-point equations for certain multiple integral representation for EFP, a conjectural expression for the limit shape of large ASMs is derived. The case of 3-enumerated ASMs is also considered.
Abstract. The problem of the limit shape of large alternating sign matrices (ASMs) is addressed by studying the emptiness formation probability (EFP) in the domain-wall six-vertex model. Assuming that the limit shape arises in correspondence to the 'condensation' of almost all solutions of the saddle-point equations for certain multiple integral representation for EFP, a conjectural expression for the limit shape of large ASMs is derived. The case of 3-enumerated ASMs is also considered.
“…Evaluating the integral in RHS of (5.13), one finds that (5.13) is nothing but the relation 16) where E denotes the lower triangular matrix, with entries standing under the main diagonal equal to one and all other entries being zeroes, i.e., E pr = δ p,r+1 . Inverting matrix A in (5.15) with the help of (5.16), one arrives immediately to the expression for H N 's, which follows from formula (5.11) and definition (5.14).…”
Section: Multiple Integral Representation Let H (R)mentioning
Abstract. The emptiness formation probability in the six-vertex model with domain wall boundary conditions is considered. This correlation function allows one to address the problem of limit shapes in the model. We apply the quantum inverse scattering method to calculate the emptiness formation probability for the inhomogeneous model. For the homogeneous model, the result is given both in terms of certain determinant and as a multiple integral representation.
“…In this section the results for one-and two-point boundary correlation functions will be analyzed by making use of the orthogonal polynomials theory, along the lines proposed in paper [27]. Here we show that the two-point boundary correlation function, studied in the previous section, is expressible in terms of one-point ones.…”
“…First we note, following paper [27], that the determinant entering the expression for the homogenous model partition function can be related with orthogonal polynomials using the integral representation…”
The six-vertex model with domain wall boundary conditions (DWBC) on an N × N square lattice is considered. The two-point correlation function describing the probability of having two vertices in a given state at opposite (top and bottom) boundaries of the lattice is calculated. It is shown that this two-point boundary correlator is expressible in a very simple way in terms of the one-point boundary correlators of the model on N × N and (N − 1) × (N − 1) lattices. In alternating sign matrix (ASM) language this result implies that the doubly refined x-enumerations of ASMs are just appropriate combinations of the singly refined ones.
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