Abstract
The following ‘partial’ integral equation arises in the quantum theory of fields:where f(x1x2) = f(x2x1), K(x1x2, y) = K(x2x1, y), and a symmetric solution of the equation is desired. The solution of (1) will be obtained as a special case of the solution of the following equation:
Publisher
Cambridge University Press (CUP)
Cited by
3 articles.
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