305 research outputs found
Rotational invariance of quadromer correlations on the hexagonal lattice
In 1963 Fisher and Stephenson \cite{FS} conjectured that the monomer-monomer
correlation on the square lattice is rotationally invariant. In this paper we
prove a closely related statement on the hexagonal lattice. Namely, we consider
correlations of two quadromers (four-vertex subgraphs consisting of a monomer
and its three neighbors) and show that they are rotationally invariant.Comment: 28 page
Macroscopically separated gaps in dimer coverings of Aztec rectangles
In this paper we determine the interaction of diagonal defect clusters in
regions of an Aztec rectangle that scale to arbitrary points on its symmetry
axis (in earlier work we treated the case when this point was the center of the
scaled Aztec rectangle). We use the resulting formulas to determine the
asymptotics of the correlation of defects that are macroscopically separated
from one another and feel the influence of the boundary. In several of the
treated situations this seems not to be accomplishable by previous methods. Our
applications include the case of two long neutral strings, which turn out to
interact by an analog of the Casimir force, two families of neutral doublets
that turn out to interact completely independently of one another, a neutral
doublet and a very long neutral string, a general collection of macroscopically
separated monomer and separation defects, and the case of long strings
consisting of consecutive monomers.Comment: 43 page
The equivalence between enumerating cyclically symmetric, self-complementary and totally symmetric, self-complementary plane partitions
We prove that the number of cyclically symmetric, self-complementary plane
partitions contained in a cube of side equals the square of the number of
totally symmetric, self-complementary plane partitions contained in the same
cube, without explicitly evaluating either of these numbers. This appears to be
the first direct proof of this fact. The problem of finding such a proof was
suggested by Stanley
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