LOG IN or SELECT A PURCHASE OPTION:
J. Math. Phys. 27, 185 (1986); http://dx.doi.org/10.1063/1.527360 (17 pages)
Continued fractions and Rayleigh–Schrödinger perturbation theory at large order
(Received 30 May 1985; accepted 10 July 1985)
Concern with the continued fraction representations of divergent Rayleigh–Schrödinger perturbation expansions in quantum mechanics is expressed. The following relation between the large‐order behavior of the continued fraction coefficients cn and the perturbation series coefficients E(n) is shown to exist: If E(n) ∼(−1)n+1Γ( pn+a), p=0,1,2,..., as n→∞, then cn=O(np) as n→∞. The case p=1 is studied in detail here, using the problems of the quartic anharmonic oscillator and the hydrogen atom in a linear radial potential as illustrative examples. For p=1 the asymptotics of the cn are shown to be linked to the infinite field limit E(λ)∼F(0)λα, predicting α and providing convergent estimates of F(0).
KEYWORDS and PACS
ARTICLE DATA
Digital Object Identifier
PUBLICATION DATA
For access to fully linked references, you need to log in.
-
C. M. Bender and T. T. Wu, Phys. Rev. 184, 1231 (1969).
C. M. Bender and T. T. Wu, Phys. Rev. Lett. 27, 461 (1971).
C. M. Bender and T. T. Wu, Phys. Rev. D 7, 1620 (1973).
J. Cizek and E. R. Vrscay, Phys. Rev. A 30, 1550 (1984).
E. R. Vrscay, Phys. Rev. A 31, 2054 (1985).
P. W. Langhoff, C. T. Corcoran, J. S. Sims, F. Weinhold, and R. M. Glover, Phys. Rev. A 14, 1042 (1976).
E. Eichten, K. Gottfried, T. Kinoshita, K. D. Lane, and T. M. Yan, Phys. Rev. D 17, 3090 (1978).
For access to citing articles, you need to log in.
















This Publication
Scitation
SPIN
Google Scholar
PubMed