𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Large-Order perturbation theory

✍ Scribed by Tai Tsun Wu


Publisher
John Wiley and Sons
Year
1982
Tongue
English
Weight
681 KB
Volume
21
Category
Article
ISSN
0020-7608

No coin nor oath required. For personal study only.

✦ Synopsis


Abstract

The original motivation for studying the asymptotic behavior of the coefficients of perturbation series came from quantum field theory. An overview is given of some of the attempts to understand quantum field theory beyond finite‐order perturbation series. At least in the case of the Thirring model and probably in general, the full content of a relativistic quantum field theory cannot be recovered from its perturbation series. This difficulty, however, does not occur in quantum mechanics, and the anharmonic oscillator is used to illustrate the methods used in large‐order perturbation theory. Two completely different methods are discussed, the first one using the WKB approximation, and a second one involving the statistical analysis of Feynman diagrams. The first one is well developed and gives detailed information about the desired asymptotic behavior, while the second one is still in its infancy and gives instead information about the distribution of vertices of the Feynman diagrams.


πŸ“œ SIMILAR VOLUMES


Perturbation theory in large order
✍ Carl M. Bender πŸ“‚ Article πŸ“… 1978 πŸ› Elsevier Science 🌐 English βš– 851 KB
Perturbation theory in large order for s
✍ Carl M. Bender πŸ“‚ Article πŸ“… 1982 πŸ› John Wiley and Sons 🌐 English βš– 545 KB

## Abstract Reasons for understanding the general problem of perturbation theory in large order are discussed. It is shown that the behavior of perturbation theory in larger order is generally very simple because it reflects just the semiclassical content of the theory. Many simple examples are giv

Infinite order perturbation theory
✍ G.G. Hall πŸ“‚ Article πŸ“… 1977 πŸ› Elsevier Science 🌐 English βš– 244 KB

A transformation of the Schrddinger equation IS demonstrated, using a factorized wavcfunction, to produce an equation whtcft IS equi~l~nt to mflnite-order perturbation theory. The fonn&sm is used to Folve wrne perturbation problems, including the quatic perturbatmn of the ~phericrtl harmonic oscdlat