Feynman parametrization: Difference between revisions

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en>David Eppstein
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Added the symmetric form of the parametrization, used in some QED papers from the 60's.
 
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'''Schwinger parametrization''' is a technique for evaluating [[loop integral]]s which arise from [[Feynman diagram]]s with one or more loops.
 
Using the well-known observation that
 
:<math>\frac{1}{A^n}=\frac{1}{(n-1)!}\int^\infty_0 du \, u^{n-1}e^{-uA},</math>
 
[[Julian Schwinger]] noticed that one may simplify the integral:
 
:<math>\int \frac{dp}{A(p)^n}=\frac{1}{\Gamma(n)}\int dp \int^\infty_0 du \, u^{n-1}e^{-uA(p)}=\frac{1}{\Gamma(n)}\int^\infty_0 du \, u^{n-1} \int dp \, e^{-uA(p)},</math>
 
for Re(n)>0.
 
Another version of Schwinger parametrization is:
 
:<math>\frac{1}{A}=-i\int^\infty_0 du \, e^{iuA},</math>
 
and it is easy to generalize this identity to n denominators.
 
See also [[Feynman parametrization]].
 
[[Category:Quantum field theory]]
 
 
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Latest revision as of 15:23, 8 November 2014

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