1981
DOI: 10.1007/bf01258900
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Schr�dinger operators with singular magnetic vector potentials

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Cited by 191 publications
(124 citation statements)
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“…(1) (The operator nature of H ω ) Under the stated assumptions, H ω is essentially self adjoint on C ∞ 0 [51]. The random potential V ω (q) is non-negative and uniformly bounded by λb + .…”
Section: Appendix a Technical Commentsmentioning
confidence: 99%
“…(1) (The operator nature of H ω ) Under the stated assumptions, H ω is essentially self adjoint on C ∞ 0 [51]. The random potential V ω (q) is non-negative and uniformly bounded by λb + .…”
Section: Appendix a Technical Commentsmentioning
confidence: 99%
“…Then we can define H a,V as the operator defined by the closure of this quadratic form. This closure is well defined [22].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Working under these minimal regularity conditions only, H. Leinfelder and C. Simader [52] were able to improve Kato's result by allowing V = V 1 + V 2 , where V 1 ≥ −c|x| 2 and V 2 is ∆-bounded with a relative bound a < 1. In particular, if V is semi-bounded below, then the above minimal regularity conditions on b and V are sufficient for essential self-adjointness (see also [23, Ch.…”
Section: Appendix C Stummel and Kato Classesmentioning
confidence: 99%
“…1]). A non-trivial technique of non-linear truncations is used in [52] to approximate functions from the maximal domain of the operator H b,V and its quadratic form by bounded functions.…”
Section: Appendix C Stummel and Kato Classesmentioning
confidence: 99%