The monomer-dimer constant of the square lattice
Find a closed form for the entropy per site of monomer-dimer configurations on the square lattice, h ≈ 0.6627989727.
Where it stands
- OpenedOct 21, 2026
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- Adopted1 merged
Place non-overlapping dominoes (dimers) on the edges of an grid and leave the other sites empty (monomers). The number of such arrangements grows like , with . Kasteleyn, Temperley and Fisher solved the case of complete domino coverings in 1961, but no closed form is known for .
Problem
Let be the rectangle in with free boundary. A configuration is a matching: a set of pairwise disjoint edges (dimers). Every uncovered vertex is a monomer. With monomer weight and dimer weight 1, the partition function is
At every matching counts once. The monomer-dimer constant is
and the limit does not depend on the boundary conditions. Find a closed-form expression for : a finite combination of algebraic numbers, standard constants such as , , , Catalan's constant and , and special functions at algebraic arguments. The defining limit, transfer-matrix eigenvalues and numerical approximations do not count.
Background
Without monomers (, and even) the model is exactly solvable. Kasteleyn, and Temperley and Fisher, showed in 1961 that the entropy per site of domino tilings is [1, 2]. With monomers present, the problem on two-dimensional lattices is #P-complete [4], and , the entropy per site at unit activity, is known only numerically.
What is known
- Butera and Pernici (2012) quote as the most precise determination, citing Baxter (1968) and Friedland and Peled (2005) [3, 5]. They also quote as the tightest bounds then known [6].
- Kong (2006) obtained from exact enumerations on strips and claimed 11 correct digits [4]. HorizonMath uses this 12-digit value as its reference.
- According to the source, no closed form is known for any , including .
What would count as progress
- A closed-form expression that matches Kong's estimate to 11 significant digits, the accuracy claimed for it, and respects the bounds above. HorizonMath's evaluator works at 100-digit precision and rejects numerical shortcuts such as quadrature, root-finding, infinite series and fitted constants; its default test asks for 20 matching digits, which no answer can reach against this 12-digit reference.
- Eleven digits is a weak filter, so new and more precise values of are valuable in their own right, for example from larger transfer-matrix or series computations.
- A proof that an expression equals , for example through an exact solution of the model at .
References
- P. W. Kasteleyn, "The statistics of dimers on a lattice", Physica 27 (1961), 1209–1225. doi:10.1016/0031-8914(61)90063-5
- H. N. V. Temperley and M. E. Fisher, "Dimer problem in statistical mechanics — an exact result", Phil. Mag. 6 (1961), 1061–1063. doi:10.1080/14786436108243366
- R. J. Baxter, "Dimers on a rectangular lattice", J. Math. Phys. 9 (1968), 650–654. doi:10.1063/1.1664623
- Y. Kong, "Monomer-dimer model in two-dimensional rectangular lattices with fixed dimer density", Phys. Rev. E 74 (2006), 061102. doi:10.1103/PhysRevE.74.061102, arXiv:cond-mat/0610690
- S. Friedland and U. N. Peled, "Theory of computation of multidimensional entropy with an application to the monomer–dimer problem", Adv. Appl. Math. 34 (2005), 486–522. doi:10.1016/j.aam.2004.08.005
- P. Butera and M. Pernici, "Yang–Lee edge singularities from extended activity expansions of the dimer density for bipartite lattices of dimensionality 2 ≤ d ≤ 7", Phys. Rev. E 86 (2012), 011104. doi:10.1103/PhysRevE.86.011104
Source
Imported from HorizonMath monomer_dimer_entropy, curated by Erik Y. Wang, Sumeet R. Motwani et al. Open according to the source as of 2026-10-20. The statement above is written in our own words; see the source for the original wording, history and discussion.