2006
DOI: 10.1090/conm/398/07484
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Kato’s inequality and asymptotic spectral properties for discrete magnetic Laplacians

Abstract: Abstract. In this paper, a discrete form of the Kato inequality for discrete magnetic Laplacians on graphs is used to study asymptotic properties of the spectrum of discrete magnetic Schrödinger operators. We use the existence of a ground state with suitable properties for the ordinary combinatorial Laplacian and semigroup domination to relate the combinatorial Laplacian with the discrete magnetic Laplacian. Our techniques yield existence and uniqueness of the fundamental solution for the heat kernel on a grap… Show more

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Cited by 48 publications
(73 citation statements)
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References 16 publications
(25 reference statements)
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“…Using the substitution t → u 2 t, we arrive at the expression log (s/u) 2 + Λ j = We can now employ bounds from Section 5 in order to determine the asymptotic behavior of (84) [15] easily extend to compute the spectrum of the Laplacian on DT B in terms of the dual lattice B * . The existence and uniqueness of the associated heat kernel on DT B follow from general results (see, e.g., [6], [7]), thus allowing one to extend the results of Section 3 above. Assume there is a one-parameter family DT B(u) of discrete tori parametrized by u ∈ Z such that B(u)/u → M as u → ∞, where M is a positive definite d × d matrix.…”
Section: The Epstein-hurwitz Zeta Functionmentioning
confidence: 72%
“…Using the substitution t → u 2 t, we arrive at the expression log (s/u) 2 + Λ j = We can now employ bounds from Section 5 in order to determine the asymptotic behavior of (84) [15] easily extend to compute the spectrum of the Laplacian on DT B in terms of the dual lattice B * . The existence and uniqueness of the associated heat kernel on DT B follow from general results (see, e.g., [6], [7]), thus allowing one to extend the results of Section 3 above. Assume there is a one-parameter family DT B(u) of discrete tori parametrized by u ∈ Z such that B(u)/u → M as u → ∞, where M is a positive definite d × d matrix.…”
Section: The Epstein-hurwitz Zeta Functionmentioning
confidence: 72%
“…If we set m V (v) = 1 for each vertex v ∈ V and m A (e) = 1 for each edge e ∈ A, then the magnetic combinatorial Laplacian is expressed by (1.4) and is discussed in Sections 1-4. This magnetic Laplacian and corresponding Schrödinger operators are considered in [B13], [DM06], [LL93].…”
Section: Properties Of Fiber Operators and An Examplementioning
confidence: 99%
“…We assume that G has bounded vertex degree: there exists a constant N > 0 such that m(x) ≤ N, for all x ∈ V . (1) In what follows, x ∼ y indicates that there is an edge that connects x and y. We will also need a set of oriented edges [y, x] : x, y ∈ V and x ∼ y}.…”
Section: The Settingmentioning
confidence: 99%
“…For the case a ≡ 1 and w ≡ 1, the definition (4) is the same as in [1]. For the case σ ≡ 1, see [2,3].…”
Section: A Magnetic Schrödinger Operatormentioning
confidence: 99%