2011
DOI: 10.5802/afst.1319
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Essential self-adjointness for combinatorial Schrödinger operators III- Magnetic fields

Abstract: We define the magnetic Schrödinger operator on an infinite graph by the data of a magnetic field, some weights on vertices and some weights on edges. We discuss essential self-adjointness of this operator for graphs of bounded degree. The main result is a discrete version of a result of two authors of the present paper.On définit l'opérateur de Schrödinger avec champ magnétique sur un graphe infini par la donnée d'un champ magnétique, de poids sur les sommets et de poids sur les arêtes. Lorsque le graphe est d… Show more

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Cited by 42 publications
(55 citation statements)
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“…This property for the magnetic Schrödinger operators on a locally finite graph was proved in [LL93], [CTT11], [HS01]. In particular, if the magnetic flux of α is zero for any cycle on Γ * , then the magnetic Schrödinger operator H α = ∆ α + Q is unitarily equivalent to the Schrödinger operator H 0 = ∆ 0 + Q without a magnetic field.…”
Section: Floquet Decomposition Of Schrödinger Operators We Introducementioning
confidence: 83%
See 1 more Smart Citation
“…This property for the magnetic Schrödinger operators on a locally finite graph was proved in [LL93], [CTT11], [HS01]. In particular, if the magnetic flux of α is zero for any cycle on Γ * , then the magnetic Schrödinger operator H α = ∆ α + Q is unitarily equivalent to the Schrödinger operator H 0 = ∆ 0 + Q without a magnetic field.…”
Section: Floquet Decomposition Of Schrödinger Operators We Introducementioning
confidence: 83%
“…Colin de Verdière, Torki-Hamza and Truc [CTT11] obtained a condition under which the magnetic Laplacian on an infinite graph is essentially self-adjoint.…”
mentioning
confidence: 99%
“…The paper [1] contains a proof of the discrete version of Kato's inequality and a study of asymptotic properties of the spectrum of a discrete magnetic Schrödinger operator. In the context of a not necessarily complete graph of bounded degree, a sufficient condition for essential selfadjointness of ∆ σ | C c (V ) in ℓ 2 w (V ) is given in [26]. A different model for discrete magnetic Laplacian was given in [27] and, for that model, the essential self-adjointness of a semi-bounded below discrete magnetic Schrödinger operator was proven.…”
Section: Background Of the Problemmentioning
confidence: 98%
“…Following [4], we understand by a magnetic potential on the set X a function θ : X × X → [−π, π] such that θ(x, y) = −θ(y, x), x, y ∈ X.…”
Section: Quadratic Formsmentioning
confidence: 99%