Following the approach of Jones, Low, and Young, a generalized O(2,l) expansion is developed for amplitudes that have a power bounded growth asymptotically. The expansion, set up in an 0(1, 1) basis, holds in a new kinematical region, where all the incoming and outgoing clusters have space-like 0(2,
A direct method for modifying certain phase-integral approximations of arbitrary order
✍ Scribed by Nanny Fröman; Per Olof Fröman
- Publisher
- Elsevier Science
- Year
- 1974
- Tongue
- English
- Weight
- 248 KB
- Volume
- 83
- Category
- Article
- ISSN
- 0003-4916
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✦ Synopsis
The approximate solution of the differential equation d'+d? + Q'(z)+ = 0 by a general modification of certain phase-integral approximations of arbitrary order is considered. A consistent modification of these higher-order phase-integral approximations is derived on the assumption that one has found a function Q&,(z) which makes the modified first-order approximation good at certain singular points of Q+), where the unmodified approximation would break down.
I. I NTRODU~TION
In recent years considerable interest has been focused on modifications of the higher-order JWKB-approximations in order to master the difficulties which often appear at the origin when these approximations are applied to radial problems [l-5]. In the present paper we shall be concerned with certain phase-integral approximations [6, 71, the higher-orders of which are related to, but not identical to the higher-order JWKB-approximations. Our aim is to expound a conceptually simple modification procedure which can be used quite generally (not only in radial problems) for making the phase-integral approximations useful at certain singular points where they would otherwise fail. The expressions obtained for the modified phase-integral approximations of any order are written in a comparatively simple form and can be given explicitly for all orders of approximation that are ever likely to be of interest in practice for solving physical problems [S, 93.
📜 SIMILAR VOLUMES
Simple final formulae are obtained for the normalization factors of wavefunctions for bound states in a one-dimensional, single-well potential, when use is made of certain arbitrary-order phase-integral approximations, which may be modified in a convenient way.