Abstract

For all odd values of m, we prove that the sequence of the numbers of near-perfect matchings on Cm x P2n+1 cylinder with a vacancy on the boundary obeys the same recurrence relation as the sequence of the numbers of perfect matchings on Cm x P2n. Further more, we prove that for all odd values of m denominator of the generating function for the total number of the near-perfect matchings on Cm x P2n+1 graph is always the square of denominator of generating function for the sequence of the numbers of perfect matchings on Cm x P2n graph, as recently conjectured by Perepechko.

Highlights

  • The monomer-dimer problem, that of counting the exact number of coverings of a rectangular lattice by a previously specified number of monomers and dimers, arises in several models in statistical physics

  • Whereas in case the number of monomers is one the term we use for these configurations is near-perfect matchings

  • This paper deals with a monomer-dimer problem on Cm × Pn graphs which shall further on be referred to as cylinders (Figure 1)

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Summary

INTRODUCTION

The monomer-dimer problem, that of counting the exact number of coverings of a rectangular lattice by a previously specified number of monomers and dimers, arises in several models in statistical physics. Let us denote by Dm ≡ (V (Dm), E(Dm)) (m ≥ 3) the digraph whose set of vertices V (Dm) consists of all the possible states of cycles Cm( j) of graph Gm,n for some perfect matching (n an arbitrary even integer) or near-perfect matching (n an arbitrary odd integer), whilst the set of edges E(Dm) is defined in the following way: there exists an edge from vertex p1 p2 . Each walk of length 2n in the digraph Dm which starts at a vertex from the set Bm∗ and ends at a vertex from the set Em defines a unique near-perfect matching of the graph Gm,2n+1 with a vacancy on the cycle Cm(1) whose state of the cycle Cm( j) for each j, where 1 ≤ j ≤ n, is exactly the word corresponding to the j-th vertex of that walk

Forming the above mentioned bijections we have that
MM L vL
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