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Schwinger parametrization is a technique for evaluating
loop integral In quantum field theory and statistical mechanics, loop integrals are the integrals which appear when evaluating the Feynman diagrams with one or more loops by integrating over the internal momenta. These integrals are used to determine counterter ...
s which arise from
Feynman diagram In theoretical physics, a Feynman diagram is a pictorial representation of the mathematical expressions describing the behavior and interaction of subatomic particles. The scheme is named after American physicist Richard Feynman, who introduc ...
s with one or more loops. Using the well-known observation that :\frac=\frac\int^\infty_0 du \, u^e^,
Julian Schwinger Julian Seymour Schwinger (; February 12, 1918 – July 16, 1994) was a Nobel Prize winning American theoretical physicist. He is best known for his work on quantum electrodynamics (QED), in particular for developing a relativistically invariant ...
noticed that one may simplify the integral: :\int \frac=\frac\int dp \int^\infty_0 du \, u^e^=\frac\int^\infty_0 du \, u^ \int dp \, e^, for Re(n)>0. Another version of Schwinger parametrization is: :\frac=\int^\infty_0 du \, e^, which is convergent as long as \epsilon >0 and A \in \mathbb R. It is easy to generalize this identity to n denominators.


See also

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Feynman parametrization Feynman parametrization is a technique for evaluating loop integrals which arise from Feynman diagrams with one or more loops. However, it is sometimes useful in integration in areas of pure mathematics as well. Formulas Richard Feynman observed ...


References

Quantum field theory {{quantum-stub