Abstract:1. There is a well-perfected Fredholm theory for singular integral operators on Rn or compact manifolds, initiated principally by Calderon and Zygmund,' and Seeley,2 which has been extended to singular integrodifferential operators, or pseudodifferential operators, by various authors.3 The presence of boundary points, however, provides considerable additional difficulties for which there does not seem to exist an equally smooth treatment, in spite of strong activity and important progress during the last 2 yea… Show more
“…Theorem 36 is proved by the same methods as applied for our earlier results concerning the algebra D. The proof is omitted. However, some details can be found in [15] since, when n 1, e is unitarily equivalent to the algebra studied there.…”
Section: (A) Any Operator a As Defined By Equationmentioning
confidence: 97%
“…To this end, we bring to bear an approach in the theory of singular integral operators which originated with Goh'berg [5] and has since been elaborated and exploited by Seeley, Breuer, and the authors [1,2,3,6,10,15].…”
Section: Gel'fand Theory Of Pseudo Differentialmentioning
“…Theorem 36 is proved by the same methods as applied for our earlier results concerning the algebra D. The proof is omitted. However, some details can be found in [15] since, when n 1, e is unitarily equivalent to the algebra studied there.…”
Section: (A) Any Operator a As Defined By Equationmentioning
confidence: 97%
“…To this end, we bring to bear an approach in the theory of singular integral operators which originated with Goh'berg [5] and has since been elaborated and exploited by Seeley, Breuer, and the authors [1,2,3,6,10,15].…”
Section: Gel'fand Theory Of Pseudo Differentialmentioning
Yes it does ! Indeed an extended version of Levinson's theorem is proposed for a system involving complex eigenvalues. The perturbed system corresponds to a realization of the Schrödinger operator with inverse square potential on the half-line, while the Dirichlet Laplacian on the half-line is chosen for the reference system. The resulting relation is an equality between the number of eigenvalues of the perturbed system and the winding number of the scattering system together with additional operators living at 0-energy and at infinite energy.
“…has for all k ∈ R 3 with k 2 = 0 a unique solution with the second term in the r.h.s. of (11) in C 0 (R 3 ) for the x-variable. Furthermore, the following asymptotic development holds:…”
Section: New Formulas For the Wave Operatorsmentioning
The paper is a presentation of recent investigations on potential scattering in R 3 . We advocate a new formula for the wave operators and deduce the various outcomes that follow from this formula. A topological version of Levinson's theorem is proposed by interpreting it as an index theorem.
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