Have You Uncovered Any Insane Integral Tricks in QFT Today?

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SUMMARY

The forum discussion centers on advanced integral techniques in Quantum Field Theory (QFT), specifically focusing on the integral transformation of the form \int \frac{d^d k}{(2\pi)^d}\frac{1}{(k^2 + m^2)^n}. The user presents a substitution involving the Gamma function, leading to a simplified result: \int \frac{d^d k}{(2\pi)^d}\frac{1}{(k^2 + m^2)^n}=\frac{\Gamma(n-d/2)(m^2)^{d/2-n}}{\Gamma(n)(4\pi)^{d/2}}. Additionally, a beta integral is derived from a combinatorial perspective, demonstrating the relationship between particle distributions and integral calculus. The discussion encourages sharing further integral tricks and hints at the potential use of Laplace transforms for solving complex integrals.

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This discussion is beneficial for theoretical physicists, mathematicians specializing in integral calculus, and advanced students in Quantum Field Theory seeking to enhance their understanding of integral techniques and transformations.

tim_lou
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Ingenious integral tricks

In QFT today I learned some insane tricks in calculating impossible integrals...I figure it'd be a good idea to see if others have similar tricks so we can all learn from each other.

here goes:
to integrate (bounds are assumed to be from negative inf to inf, k^2 means the vector dot product)
edit: missing factors of 2pi

[tex]\int \frac{d^d k}{(2\pi)^d}\frac{1}{(k^2 + m^2)^n}[/tex]
substitute
[tex]\frac{1}{(k^2 + m^2)^n}=\frac{1}{\Gamma(n)}\int_0^\infty t^n e^{-t(k^2 + m^2)} dt[/tex]

and get a gaussian in the integral. At the end of the day,
[tex]\int \frac{d^d k}{(2\pi)^d}\frac{1}{(k^2 + m^2)^n}=\frac{\Gamma(n-d/2)(m^2)^{d/2-n}}{\Gamma(n)(4\pi)^{d/2}}[/tex]

[tex]\Gamma(n)=(n-1)![/tex]

Quite crazy eh? I would've never thought of it myself... what about your favorite crazy tricks?
 
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Another I have to share (I read it in some analysis book...)

take the following integral
[tex]\binom{m+n+1}{m,n}\int_0^1 u^{m} (1-u)^n du[/tex]
consider the integral as a sum, we see that given m+n+1 particles on (0,1), it sums the probability of finding m particles in (0, u), 1 particle around the point u and n particles in (u, 1), so it must be one. This gives the beta integral for integers m, n!
[tex]\int_0^1 u^{m} (1-u)^n du=\frac{m!n!}{(m+n+1)!}[/tex]
 


tim_lou said:
substitute
[tex]\frac{1}{(k^2 + m^2)^n}=\frac{1}{\Gamma(n)}\int_0^\infty t^n e^{-t(k^2 + m^2)} dt[/tex]

I wonder if most of these crazy tricks can be found without guessing. This substitution suggests that the initial problem could be simply solved by Laplace transforms?!
 

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