Abstract
Let H(0) be a dilation-analytic three-particle Schrödinger operator with analytic continuation H(ϕ) (ϕ>0). Let a be zero or the energy of a two-particle bound state. Let-Δ (a) be the Laplace operator representing the kinetic energy of the relative motion of fragments scattered in channel a. By recent results, wave operators W (±, a, ϕ) with conjugates W† (±, a, ϕ) exist such that W (±, a, ϕ) W† (±, a, ϕ) is a projection P (a, ϕ) commuting with H (ϕ) while [H (ϕ)-a]W (±, a, ϕ) equals-W(±, a, ϕ) Δ (a) e2iϕ. This paper shows that the wave operators transform dilation-analytic functions of particle coordinates into dilation-analytic functions. Specifically, if the left shoulder of the spectrum of P (a,ϕ) H (ϕ) does not sweep across eigenvalues of H(ϕ) when α≤ϕ≤β, then W(-, a, ϕ) and W† (+, a, ϕ) are dilation analytic in [α, β]. If the right shoulder does not sweep across eigenvalues, W(+, a, ϕ) and W†(-, a, ϕ) are dilation analytic in [α,β]. A semisimple eigenvalue of H (ψ) embedded in the spectrum of P (a, ψ) H (ψ) does not prevent the wave operators from being dilation analytic in an interval [α, β] with ψ as an interior point.
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This work was supported in part by the National Science Foundation under grant DMS-8301096.
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van Winter, C. Dilation-analytic wave operators for three particles. Integr equ oper theory 9, 387–451 (1986). https://doi.org/10.1007/BF01199352
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DOI: https://doi.org/10.1007/BF01199352