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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


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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,

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✍ Per Olof Fröman 📂 Article 📅 1974 🏛 Elsevier Science 🌐 English ⚖ 478 KB

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.