Abstract

The problem of counting monomer-dimer coverings of a lattice is a longstanding problem in statistical mechanics.It has only been exactly solved for the special case of dimer coverings in two dimensions ([Ka61], [TF61]). In earlier work, Stanley [St85] proved a reciprocity principle governing the number $N(m,n)$ of dimer coverings of an $m$ by $n$ rectangular grid (also known as perfect matchings), where $m$ is fixed and $n$ is allowed to vary. As reinterpreted by Propp [P01], Stanley's result concerns the unique way of extending $N(m,n)$ to $n<0$ so that the resulting bi-infinite sequence, $N(m,n)$ for $n \in \mathbb{Z}$, satisfies a linear recurrence relation with constant coefficients. In particular, Stanley shows that $N(m,n)$ is always an integer satisfying the relation $N(m,-2-n) = \varepsilon_{m,n} N(m,n)$ where $\varepsilon_{m,n}=1$ unless $m \equiv 2(\mod 4)$ and $n$ is odd, in which case $\varepsilon_{m,n}=-1$. Furthermore, Propp's method was applicable to higher-dimensional cases.This paper discusses similar investigations of the numbers $M(m,n)$, of monomer-dimer coverings, or equivalently (not necessarily perfect) matchings of an $m$ by $n$ rectangular grid. We show that for each fixed $m$ there is a unique way of extending $M(m,n)$ to $n<0$ so that the resulting bi-infinite sequence, $M(m,n)$ for $n \in \mathbb{Z}$, satisfies a linear recurrence relation with constant coefficients.We show that $M(m,n)$, a priori a rational number, is always an integer, using a generalization of the combinatorial model offered by Propp. Lastly, we give a new statement of reciprocity in terms of multivariate generating functions from which Stanley's result follows.

Highlights

  • The problem of counting the number of monomer-dimer coverings of a lattice has been examined for many years in the field of statistical mechanics (see (KRS96)), and has applications in biology, chemistry and physics

  • While we cannot offer an exact solution to the monomer-dimer problem, we can express a symmetry relationship between the numbers of coverings of certain families of lattices; the base case being a rectangular grid of

  • The numbers an satisfy a linear recurrence which we can use to compute the numbers a0, a−1, a−2, . . . Surprisingly, we find that the new numbers are related, term by term, to the original sequence of numbers; for instance an ∼ a−n−2

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Summary

A Reciprocity Theorem for Monomer-Dimer Coverings

To cite this version: Nick Anzalone, John Baldwin, Ilya Bronshtein, Kyle Petersen. A Reciprocity Theorem for MonomerDimer Coverings. The problem of counting monomer-dimer coverings of a lattice is a longstanding problem in statistical mechanics. Stanley (Sta85) proved a reciprocity principle governing the number N(m, n) of dimer coverings of an m by n rectangular grid ( known as perfect matchings), where m is fixed and n is allowed to vary. As reinterpreted by Propp (Pro01), Stanley’s result concerns the unique way of extending N(m, n) to n < 0 so that the resulting biinfinite sequence, N(m, n) for n ∈ Z, satisfies a linear recurrence relation with constant coefficients. We show that for each fixed m there is a unique way of extending M(m, n) to n < 0 so that the resulting bi-infinite sequence, M(m, n) for n ∈ Z, satisfies a linear recurrence relation with constant coefficients. We give a new statement of reciprocity in terms of multivariate generating functions from which Stanley’s result follows

Background
The Problem
Signed Graphs and Signed Matchings
Adjunction
Combinatorial Reciprocity
The Generating Function
More on Linear Recurrences and Reciprocity
Full Text
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