2015
DOI: 10.1016/j.laa.2013.12.039
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Green matrices associated with generalized linear polyominoes

Abstract: A Polyomino is an edge-connected union of cells in the planar square lattice. Here we consider generalized linear polyominoes; that is, the polyominoes supported by a n × 2 lattice. In this paper, we obtain the Green function and the Kirchhoff index of a generalized linear polyomino as a perturbation of a 2n-path by adding weighted edges between opposite vertices. This approach deeply links generalized linear polyomino Green functions with the inverse M-matrix problem, and especially with the so-called Green m… Show more

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Cited by 8 publications
(3 citation statements)
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“…Since the cycle is obtained from the path by adding a new edge, we can see it as a perturbation of the path. Specifically, we analyze here the perturbation of the signless Laplacian of the path, since the perturbation of the combinatorial Laplacian has been treated in other works, see [5]. Recall that the path is always bipartite, and hence its signless Laplacian is singular and elliptic, but the cycle is elliptic only when the number of vertices is even.…”
Section: Perturbation Of Elliptic Schrödinger-like Operatorsmentioning
confidence: 99%
“…Since the cycle is obtained from the path by adding a new edge, we can see it as a perturbation of the path. Specifically, we analyze here the perturbation of the signless Laplacian of the path, since the perturbation of the combinatorial Laplacian has been treated in other works, see [5]. Recall that the path is always bipartite, and hence its signless Laplacian is singular and elliptic, but the cycle is elliptic only when the number of vertices is even.…”
Section: Perturbation Of Elliptic Schrödinger-like Operatorsmentioning
confidence: 99%
“…In [23] we presented an algorithm for solving the forward problem of determining u, given η. Our approach was a perturbative one, making use of known Green's functions for the time-independent diffusion equation (or Schrödinger equation) [3,8,9,7,12,13,14,15,40,42], with η identically zero. The corresponding inverse problem, which we refer to as graph optical tomography, is to recover the potential η from measurements of u on the boundary of the graph.…”
Section: Introductionmentioning
confidence: 99%
“…Then, we can consider c 1 , c 2 as the boundary conditions with coefficients σ 11 , σ 12 , σ 13 , σ 14 and σ 21 , σ 22 , σ 23 , σ 24 , respectively, and we denote with (c 1 , c 2 ) the pair of boundary conditions determined by the matrix C = With this all functional notation, (2) and (3) are equivalent to the boundary value problem on the path I L γ q (u) = f on • I, c 1 (u) = f (0) and c 2 (u) = f (n + 1). (5) In terms of the boundary value problem, the invertibility conditions for M are exactly the same conditions to ensure that the above boundary value problem is regular, that is, it has a unique solution for each given data. Therefore, the computation of the inverse of M can be reduced to the calculus of the solution of boundary value problems for suitable data.…”
mentioning
confidence: 99%