How Does Dimensional Regularization Simplify Integrals in Quantum Field Theory?

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how does dimensional regularization work ?

i see , how can you calculate integrals in d-dimensions of the form

\int d^{d} k F( \vec k ) ??

and for other cases , let us suppose we have the integral

\lim_{\varepsilon\rightarrow 0^+}\int \frac{dp}{(2\pi)^{4-\varepsilon}} \frac{2\pi^{(4-\varepsilon)/2}}{\Gamma\left(\frac{4-\varepsilon}{2}\right)} \frac{p^{3-\varepsilon}}{\left(p^2+m^2\right)^1}

there is no way this integral can be calculated
 
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It works by analytic continuation. Consider the integral

\int_0^\infty dx\,{x^n\over x^2+1}.

For -1<{\rm Re}\,n<1, the integral converges, and the result is

{\pi/2\over\cos(n\pi/2)}.

We now define this to be the value of the integral for all n.
 
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