Hostname: page-component-586b7cd67f-r5fsc Total loading time: 0 Render date: 2024-11-23T17:44:00.620Z Has data issue: false hasContentIssue false
  • English
  • Français

The bound state representation

Published online by Cambridge University Press:  24 October 2008

J. Hamilton  and
A. Salam
J. Hamilton
Affiliation:
Christ's CollegeCambridge
A. Salam
Affiliation:
St John's CollegeCambridge
Get access Rights & Permissions [Opens in a new window]

Abstract

Eigenvalues and eigenvectors of the total Hamiltonian in field theory are determined by the method of direct diagonalization, using canonical transformations. The difficulties of this method are discussed in detail.

Type
Research Article
Information
Mathematical Proceedings of the Cambridge Philosophical Society , Volume 51 , Issue 1 , January 1955 , pp. 103 - 112
Copyright
Copyright © Cambridge Philosophical Society 1955

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

(1)Dancoff, S. M.Phys. Rev. 78 (1950), 382.CrossRefGoogle Scholar
(2)Dyson, F. J.Phys. Rev. 83 (1951), 608, 1207.Google Scholar
(3)Dyson, F. J.Phys. Rev. 90 (1953), 994.CrossRefGoogle Scholar
(4)Gell-Mann, M. and Low, F.Phys. Rev. 84 (1951), 350.CrossRefGoogle Scholar
(5)Heitler, W.Quantum theory of radiation, 3rd ed. (Oxford, 1954).Google Scholar
(6)Levy, M. M.Phys. Rev. 88 (1952), 725.CrossRefGoogle Scholar
(7)Ma, S. T.Phys. Rev. 87 (1952), 652.Google Scholar
(8)Matthews, P. T. and Salam, A.Proc. roy. Soc. A, 221 (1953), 128.Google Scholar
(9)Salpeter, E. E. and Bethe, H. A.Phys. Rev. 84 (1951), 1232.CrossRefGoogle Scholar
(10)Schwinger, J.Phys. Rev. 75 (1949), 651.Google Scholar
(11)Tamm, I.J. Phys., Moscow, 9 (1945), 449.Google Scholar
(12)Taylor, J. C.Phys. Rev. 95 (1954), 1313.CrossRefGoogle Scholar