Abstract:We analyse the spectrum of a self-adjoint operator on a Laakso space using the projective limit construction originally given by Barlow and Evans. We will use the hierarchical cell structure induced by the choice of approximating quantum graphs to calculate the spectrum with multiplicities. We also extend the method for using the hierarchical cell structure to more general projective limits beyond Laakso spaces.
“…Then in [16], a more in depth description of the projective limit construction was used to calculate the spectrum of the Laplacian constructed in [17]. We will be using the construction in [16] as it is also well-suited for our calculations.…”
Section: Laakso Spacesmentioning
confidence: 99%
“…In Section 3.1 we provide an analytical proof by examining, as in [16], the different "shapes" that make up the space. Since each shape has a unique contribution to the spectrum counting the number of shapes allows us to calculate the spectrum with multiplicities.…”
Section: Introductionmentioning
confidence: 99%
“…We begin by reviewing the construction of the Laakso spaces as presented in [11,16,17] in Section 2. This section also contains background information on the Hausdorff dimension, its calculation for Laakso spaces, and some specific values for certain Laakso spaces.…”
Section: Introductionmentioning
confidence: 99%
“…This paper will be concerned instead with the irregular domain being a fractal itself. Some notable works with this type of domain include [3,6,8,16,17,19] among others. Laakso's spaces were introduced in [11].…”
Section: Introductionmentioning
confidence: 99%
“…They are a family of fractals with an arbitrary Hausdorff dimension greater than one and were considered originally for their nice analytic properties. Constructions of the Laakso spaces are given in [11,16,17] as well as in Section 2 of this paper. Theorem 6.1 in [16] gives the spectrum of the Laplacian operator on any given Laakso space, in Theorem 3.1 we give the multiplicities.…”
We introduce a method of constructing a general Laakso space while calculating the spectrum and multiplicities of the Laplacian operator on it. Using this information, we find the leading term of the trace of the heat kernel and the spectral dimension on an arbitrary Laakso space.
“…Then in [16], a more in depth description of the projective limit construction was used to calculate the spectrum of the Laplacian constructed in [17]. We will be using the construction in [16] as it is also well-suited for our calculations.…”
Section: Laakso Spacesmentioning
confidence: 99%
“…In Section 3.1 we provide an analytical proof by examining, as in [16], the different "shapes" that make up the space. Since each shape has a unique contribution to the spectrum counting the number of shapes allows us to calculate the spectrum with multiplicities.…”
Section: Introductionmentioning
confidence: 99%
“…We begin by reviewing the construction of the Laakso spaces as presented in [11,16,17] in Section 2. This section also contains background information on the Hausdorff dimension, its calculation for Laakso spaces, and some specific values for certain Laakso spaces.…”
Section: Introductionmentioning
confidence: 99%
“…This paper will be concerned instead with the irregular domain being a fractal itself. Some notable works with this type of domain include [3,6,8,16,17,19] among others. Laakso's spaces were introduced in [11].…”
Section: Introductionmentioning
confidence: 99%
“…They are a family of fractals with an arbitrary Hausdorff dimension greater than one and were considered originally for their nice analytic properties. Constructions of the Laakso spaces are given in [11,16,17] as well as in Section 2 of this paper. Theorem 6.1 in [16] gives the spectrum of the Laplacian operator on any given Laakso space, in Theorem 3.1 we give the multiplicities.…”
We introduce a method of constructing a general Laakso space while calculating the spectrum and multiplicities of the Laplacian operator on it. Using this information, we find the leading term of the trace of the heat kernel and the spectral dimension on an arbitrary Laakso space.
We investigate the existence of the meromorphic extension of the spectral zeta function of a Laplacian on self-similar fractals using the results of Kigami and Lapidus (based on renewal theory) and the newer results by Hambly and Kajino based on heat kernel estimates and other probabilistic techniques. We also formulate conjectures which hold true for the examples that have been analyzed in the existing literature.
We consider the spaces introduced by Laakso in 2000 and, building on the work of Barlow, Bass, Kumagai, and Teplyaev, prove the existence and uniqueness of a local symmetry invariant diffusion via heat kernel estimates.
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