The Gauß-Bonnet operator of an infinite graph
Résumé
We propose a general condition for selfadjointness of the Gauß-Bonnet operator D=d+delta based on the notion of negligible boundary introduced by Gaffney. This gives self-adjointness of the Laplace operator both for functions or 1-forms on infinite graphs. This is used to extend Flanders result concerning solutions of Kirchhoff laws.
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