Abstract
The stationary Schrödinger equation is ∂ 2x φ + λV(x)φ=zφ for φ∈ℒ2(R +,dx). If the potential is bounded below, singular only atx=0, negative on some compact interval and behaves likeV(x)∼1/x μ asx→∞ with 2≧μ>0, then the system admits shape resonances which continuously become eigenvalues as λ increases. Here λ>0 and for μ=2 a sufficiently large λ is required. Exponential bounds are obtained on Im(z) as λ approaches a threshold. The group velocity near threshold is also estimated.
Similar content being viewed by others
References
Comes, J.M., Hislop, P.D.: Stark ladder resonances for small electric fields. Commun. Math. Phys.140, 291–320 (1991)
Hislop, P.D., Sigal, I.M.: Semi-classical theory of shape resonances in quantum mechanics. Memoirs of the AMS, Vol.78, 399 (1989)
Klaus, M., Simon, B.: Coupling constant thresholds in non-relativistic quantum mechanics. Ann. Phys., Vol.130 (2), 251–281 (1980)
Pravica, D.W.: Trapped rays in cylindrically symmetric media and poles of the analytically continued resolvent. J. Math. Anal. Appl., to Appear
Pravica, D.W.: Shape resonances: A comparison between parabolic and flat potentials. J. Diff. Eq., Vol.129 (2), 262–289 (1996)
Rauch, J.: Perturbation theory for eigenvalues and resonances of Schrödinger Hamiltonians. J. Funct. Anal., Vol.35, 304–315 (1980)
Reed, M., Simon, B.: Methods of Modern Mathematical Physics: IV—Analysis of Operators. London: Acad. Pr., 1979
Sigal, I.M.: Sharp exponential bounds on resonance states and width of resonances, Adv. Appl. Math., Vol.9, 127–166 (1988)
Author information
Authors and Affiliations
Additional information
Communicated by B. Simon
Rights and permissions
About this article
Cite this article
Pravica, D.W. Spectral resonances which become eigenvalues. Commun.Math. Phys. 182, 661–673 (1996). https://doi.org/10.1007/BF02506421
Received:
Accepted:
Issue Date:
DOI: https://doi.org/10.1007/BF02506421