Abstract:Abstract. Let H 0 and H be a pair of self-adjoint operators satisfying some standard assumptions of scattering theory. It is known from previous work that if λ belongs to the absolutely continuous spectrum of H 0 and H, then the difference of spectral projectionsin general is not compact and has non-trivial absolutely continuous spectrum. In this paper we consider the compact approximations D ε (λ) of D(λ), given bywhere ψ ε (x) = ψ(x/ε) and ψ(x) is a smooth real-valued function which tends to ∓1/2 as x → ±∞. … Show more
“…Yet another example is the discrete Laplacian. We omit the details, but refer to Section 11 of [14] for some of the necessary ingredients for these extensions in some cases.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The discontinuous limiting function is f (x) = χ {x<µ} , while the functions approximating this function can be chosen smooth; see Section 3 in [8]. To be more precise, in this problem the product of f (H 1 ) and f (H 0 ) rather than their difference appears, but a mathematically closely related problem for the difference was studied by one of us in [14]. In fact, in view of the latter work we believe that for both the operator norm and the Schatten norm with any fixed 0 < p < ∞ the assumptions on ρ and f in Theorems 1.1 and 1.2 are best possible.…”
We consider the difference f (H 1 ) − f (H 0 ), where H 0 = −∆ and H 1 = −∆ + V are the free and the perturbed Schrödinger operators in L 2 (R d ), and V is a real-valued short range potential. We give a sufficient condition for this difference to belong to a given Schatten class S p , depending on the rate of decay of the potential and on the smoothness of f (stated in terms of the membership in a Besov class). In particular, for p > 1 we allow for some unbounded functions f .
“…Yet another example is the discrete Laplacian. We omit the details, but refer to Section 11 of [14] for some of the necessary ingredients for these extensions in some cases.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The discontinuous limiting function is f (x) = χ {x<µ} , while the functions approximating this function can be chosen smooth; see Section 3 in [8]. To be more precise, in this problem the product of f (H 1 ) and f (H 0 ) rather than their difference appears, but a mathematically closely related problem for the difference was studied by one of us in [14]. In fact, in view of the latter work we believe that for both the operator norm and the Schatten norm with any fixed 0 < p < ∞ the assumptions on ρ and f in Theorems 1.1 and 1.2 are best possible.…”
We consider the difference f (H 1 ) − f (H 0 ), where H 0 = −∆ and H 1 = −∆ + V are the free and the perturbed Schrödinger operators in L 2 (R d ), and V is a real-valued short range potential. We give a sufficient condition for this difference to belong to a given Schatten class S p , depending on the rate of decay of the potential and on the smoothness of f (stated in terms of the membership in a Besov class). In particular, for p > 1 we allow for some unbounded functions f .
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