1985
DOI: 10.2977/prims/1195179628
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Examples of Absolutely Continuous Schrödinger Operators in Magnetic Fields

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Cited by 64 publications
(78 citation statements)
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“…Second, if we suppose that b ∈ C 1 (R), it follows from the above remark and Lemma 5.2 that the band functions are non constant with no constraint on . We mention that Iwatsuka [12] proves absolutely continuity of the spectrum provided the magnetic field b(x) is smooth b(x) ∈ C ∞ (R), it is bounded 0 < M − b(x) M + < ∞, and lim sup x→−∞ b(x) < lim inf x→∞ b(x) or the reverse inequality. Furthermore, under the additional condition that b(x) is monotone (without any regularity assumption), Dombrowski, Germinet, and Raikov [6, Corollary 2.3] proved the quantization of the edge current (see section 1.1).…”
Section: 21mentioning
confidence: 99%
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“…Second, if we suppose that b ∈ C 1 (R), it follows from the above remark and Lemma 5.2 that the band functions are non constant with no constraint on . We mention that Iwatsuka [12] proves absolutely continuity of the spectrum provided the magnetic field b(x) is smooth b(x) ∈ C ∞ (R), it is bounded 0 < M − b(x) M + < ∞, and lim sup x→−∞ b(x) < lim inf x→∞ b(x) or the reverse inequality. Furthermore, under the additional condition that b(x) is monotone (without any regularity assumption), Dombrowski, Germinet, and Raikov [6, Corollary 2.3] proved the quantization of the edge current (see section 1.1).…”
Section: 21mentioning
confidence: 99%
“…Iwatsuka [12] studied the case when the magnetic field is not constant at infinity. In particular, he considered the case when b(x, y) = b(x) is a function of x only.…”
Section: Introduction: Magnetic Barriers and Edge Currentsmentioning
confidence: 99%
“…[54, Thm. XIII.86] and [28,Lemma 2.6]) that the nth band contributes to the absolutely continuous spectrum of H(b). In the other case, |β n | = 0, the nth band contributes to the pure-point spectrum of H(b) [54, Thm.…”
Section: Definition 21 (Umf) a Unidirectionally Constant Magnetic Fmentioning
confidence: 99%
“…The quantum analogue of this unbounded motion should manifest itself in the exclusive appearence of absolutely continuous spectrum of the underlying one-particle Schrödinger operator with a UMF (only), which is not globally constant. Although plausible from the (quasi-) classical picture, a mathematical proof of this conjecture is nontrivial and has been accomplished so far only for certain classes of UMF's [28,45]. From the same picture, the absolutely continuous spectrum should come with ballistic transport along the direction perpendicular to the gradient of the UMF.…”
Section: Introductionmentioning
confidence: 99%
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