2006
DOI: 10.1016/j.crma.2006.11.001
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On the essential spectrum of magnetic pseudodifferential operators

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Cited by 18 publications
(36 citation statements)
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“…To give a better idea of the meaning of holes death, let us consider some example. The smallest cycle in H 1 is an empty triangle, one of such cycles is given by the three simplices {(Schur's lemma, Stone-Von Neumann Theorem), (Schur's lemma, Spectral Theorem), (Spectral Theorem, Stone-Von Neumann Theorem)} which is killed by a 2-simplex when the three concepts appear together in the paper [20]. Another interesting example is a 5-step long cycle in [13].…”
Section: Resultsmentioning
confidence: 99%
“…To give a better idea of the meaning of holes death, let us consider some example. The smallest cycle in H 1 is an empty triangle, one of such cycles is given by the three simplices {(Schur's lemma, Stone-Von Neumann Theorem), (Schur's lemma, Spectral Theorem), (Spectral Theorem, Stone-Von Neumann Theorem)} which is killed by a 2-simplex when the three concepts appear together in the paper [20]. Another interesting example is a 5-step long cycle in [13].…”
Section: Resultsmentioning
confidence: 99%
“…To include a variable magnetic field, one must introduce a "twisted" form of the Weyl calculus [13,14,15], obtaining a quantization of observables which is invariant under gauge transformations. This realization is based on twisting both the pseudo-differential calculus and the crossed products algebras by a 2-cocycle defined on the group R n with values in the unitary elements of the algebra A .…”
Section: Introductionmentioning
confidence: 99%
“…Hopefully, in some subsequent publication, we will restrict to smaller classes of groups allowing a deeper analytical investigation, involving more realistic spaces of functions. For G = R n and for magnetic-type cocycles this has been undertaken in [11,12] and spectral results for magnetic Hamiltonians are contained in [14].Let us describe the content. We start exposing briefly the C * -algebraic formalism of twisted crossed products and its representation theory.…”
mentioning
confidence: 99%
“…Starting from a twisted C * -dynamical system, one can construct twisted crossed product C * -algebras [19,20,15] (see also references therein). Let L 1 (X ; A) be the complex vector space of A-valued Bochner integrable functions on X and L 1 -norm…”
Section: Magnetic Twisted Crossed Productsmentioning
confidence: 99%