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Published October 15, 1951 | Published
Journal Article Open

Bound States in Quantum Field Theory

Abstract

The relativistic two-body equation of Bethe and Salpeter is derived from field theory. It is shown that the Feynman two-body kernel may be written as a sum of wave functions over the states of the system. These wave functions depend exponentially on the energies of the states to which they correspond and therefore provide a means of calculating energy levels of bound states.

Additional Information

© 1951 American Physical Society. Received June 13, 1951. Published 15 October 1951. The authors wish to express their gratitude to Dr. J. R. Oppenheimer and to the Institute for Advanced Study for their kind hospitality. They would also like to thank the members of the Institute for many interesting discussions.

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Published - PhysRev.84.350.pdf

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August 19, 2023
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