2018
DOI: 10.3934/dcdss.2020243
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On absence of threshold resonances for Schrödinger and Dirac operators

Abstract: Using a unified approach employing a homogeneous Lippmann-Schwinger-type equation satisfied by resonance functions and basic facts on Riesz potentials, we discuss the absence of threshold resonances for Dirac and Schrödinger operators with sufficiently short-range interactions in general space dimensions. More specifically, assuming a sufficient power law decay of potentials, we derive the absence of zero-energy resonances for massless Dirac operators in space dimensions n 3, the absence of resonances at ±m fo… Show more

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Cited by 4 publications
(6 citation statements)
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“…In fact, for n = 3 the absence of zero-energy resonances has been shown under the weaker decay [8]. The absence of zeroenergy resonances for massless Dirac operators in dimensions n 4 as contained in Theorem 10.7 (ii) appears to have gone unnoticed in the literature and was only recently observed in [83]. ⋄…”
Section: Lemma 102 ([98]mentioning
confidence: 89%
See 1 more Smart Citation
“…In fact, for n = 3 the absence of zero-energy resonances has been shown under the weaker decay [8]. The absence of zeroenergy resonances for massless Dirac operators in dimensions n 4 as contained in Theorem 10.7 (ii) appears to have gone unnoticed in the literature and was only recently observed in [83]. ⋄…”
Section: Lemma 102 ([98]mentioning
confidence: 89%
“…This is the first result of this kind applicable to non-Fredholm operators in a partial differential operator setting involving multi-dimensional massless Dirac operators. In a sense, a project that started with Pushnitski in 2008, was considerably extended in scope in [77], and further developed with the help of [38]- [44], [82], [83], finally comes full circle.…”
Section: Introductionmentioning
confidence: 99%
“…Let us mention the dichotomy between a virtual level and an eigenvalue manifested in the large-time behavior of the heat kernel and the behavior of the Green function near criticality; see [Pin92,Pin04]. We also mention recent articles [BBV20] on properties of virtual states of selfadjoint Schrödinger operators and [GN20] proving the absence of genuine (non-L 2 ) virtual states of selfadjoint Schrödinger operators and massive and massless Dirac operators, as well as giving classification of virtual levels and deriving properties of eigenstates and virtual states.…”
Section: Virtual Levelsmentioning
confidence: 99%
“…For more details and references, see [BC21]. Related results on properties of eigenstates and virtual states are in [GN20] (Schrödinger and massive Dirac operators in dimension d ≥ 3 and massless Dirac operators in d ≥ 2) and in [BBV20, Theorem 2.3] (Schrödinger operators in d ≤ 2). Let us note that, prior to [BC21], the nonselfadjoint case has not been considered (although some results appeared in [CP05]).…”
Section: Application To the Schrödinger Operatorsmentioning
confidence: 99%
“…I H 2 ; H 1 /, denoted by L .0 C I H 2 ; H 1 /, and L .0 C I H This is the first result of this kind applicable to non-Fredholm operators in a partial differential operator setting involving multi-dimensional massless Dirac operators. In a sense, a project that started with Pushnitski in 2008, was considerably extended in scope in [78], and further developed with the help of [38,[41][42][43][44]82,83], finally comes full circle.…”
Section: Introductionmentioning
confidence: 99%