Abstract

In this paper we discuss the electromagnetic field, as perturbed by a prescribed current. All quantities of physical interest in various situations, eigenvalues, eigenfunctions, and transition probabilities, are derived from a general transformation function which is expressed in a non-Hermitian representation. The problems treated are: the determination of the energy-momentum eigenvalues and eigenfunctions for the isolated electromagnetic field, and the energy eigenvalues and eigenfunctions for the field perturbed by a time-independent current; the evaluation of transition probabilities and photon number expectation values for a time-dependent current that departs from zero only within a finite time interval, and for a time-dependent current that assumes non-vanishing time-independent values initially and finally. The results are applied in a discussion of the infrared catastrophe and of the adiabatic theorem. It is shown how the latter can be exploited to give a uniform formulation for all problems requiring the evaluation of transition probabilities or eigenvalue displacements.

Keywords

EigenfunctionEigenvalues and eigenvectorsPhysicsHermitian matrixAdiabatic processCurrent (fluid)Electromagnetic fieldMomentum (technical analysis)Field (mathematics)Quantum mechanicsMathematicsPure mathematics

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Publication Info

Year
1953
Type
article
Volume
91
Issue
3
Pages
728-740
Citations
215
Access
Closed

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Cite This

Julian Schwinger (1953). The Theory of Quantized Fields. III. Physical Review , 91 (3) , 728-740. https://doi.org/10.1103/physrev.91.728

Identifiers

DOI
10.1103/physrev.91.728