Condensed Matter Physics and Exactly Soluble Models 2004
DOI: 10.1007/978-3-662-06390-3_34
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Solution of the Dimer Problem by the Transfer Matrix Method

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Cited by 12 publications
(20 citation statements)
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“…The 1-dimensional case is easy, namely e h is equal to the spectral radius ρ(A) of a certain matrix A called the "transfer matrix". There are very few 2-dimensional models where the value of h is known in closed form [2,10,23,26,27]. In all other cases there are estimates based on: (a) asymptotic expansions, e.g., [1,17,29]; (b) Monte Carlo methods, e.g., [3,20]; (c) bounds, e.g., [6,7,11,19,28,30].…”
Section: Introductionmentioning
confidence: 99%
“…The 1-dimensional case is easy, namely e h is equal to the spectral radius ρ(A) of a certain matrix A called the "transfer matrix". There are very few 2-dimensional models where the value of h is known in closed form [2,10,23,26,27]. In all other cases there are estimates based on: (a) asymptotic expansions, e.g., [1,17,29]; (b) Monte Carlo methods, e.g., [3,20]; (c) bounds, e.g., [6,7,11,19,28,30].…”
Section: Introductionmentioning
confidence: 99%
“…See for example [1,2,4,5,6,12,14,15,16,17,19,20,21,23,24,25,26,28,30]. Let G = (V, E) be an undirected graph with vertices V and edges E. G can be a finite or infinite graph.…”
Section: Introductionmentioning
confidence: 99%
“…However, in our computations m can be any natural number up to 30, so M can have 2 30 × 2 30 = 2 60 ≈ 10 18 entries. Luckily, the matrix M is highly structured (see [24]), so there exists a faster algorithm for computing P (m,n+1) from P (m,n) .…”
Section: 2mentioning
confidence: 99%