- #1
nklohit
- 13
- 0
Hi all, I have just started to study QFT myself with Srednicki's book but there are some points that aren't clear to me.
First, I search for the proof of the integral in eq. 14.27
[tex] \int \frac{d^{d}\bar{q}}{(2\pi)^d} \frac{(\bar{q}^2)^a}{(\bar{q}^2+D)^b} = \frac{\Gamma(b-a-\frac{d}{2})\Gamma(a+\frac{d}{2})}{(4\pi)^{d/2}\Gamma(b)\Gamma(\frac{d}{2})} [/tex]
but find nothing about it. Can anyone give a hint how to prove it?
Second, I'm very confusing that instead of putting the cut-off into the integration of feynman propagator, he use the factor [tex] (\frac{\Lambda^2}{k^2+\Lambda^2 -i\epsilon})[/tex] . Are there any reasons to do that?
Thank you for every answer :)
First, I search for the proof of the integral in eq. 14.27
[tex] \int \frac{d^{d}\bar{q}}{(2\pi)^d} \frac{(\bar{q}^2)^a}{(\bar{q}^2+D)^b} = \frac{\Gamma(b-a-\frac{d}{2})\Gamma(a+\frac{d}{2})}{(4\pi)^{d/2}\Gamma(b)\Gamma(\frac{d}{2})} [/tex]
but find nothing about it. Can anyone give a hint how to prove it?
Second, I'm very confusing that instead of putting the cut-off into the integration of feynman propagator, he use the factor [tex] (\frac{\Lambda^2}{k^2+\Lambda^2 -i\epsilon})[/tex] . Are there any reasons to do that?
Thank you for every answer :)