How Does Dimensional Regularization Simplify Integrals in Quantum Field Theory?

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SUMMARY

Dimensional regularization simplifies integrals in Quantum Field Theory by allowing calculations in d-dimensions, particularly for divergent integrals. The technique employs analytic continuation to define integrals that converge for certain values of n, such as the integral \(\int_0^\infty dx\,{x^n\over x^2+1}\), which yields \(\frac{\pi/2}{\cos(n\pi/2)}\) for \(-1<\text{Re}\,n<1\). This method is crucial for evaluating integrals like \(\lim_{\varepsilon\rightarrow 0^+}\int \frac{dp}{(2\pi)^{4-\varepsilon}} \frac{2\pi^{(4-\varepsilon)/2}}{\Gamma\left(\frac{4-\varepsilon}{2}\right)} \frac{p^{3-\varepsilon}}{\left(p^2+m^2\right)^1}\), which cannot be computed directly.

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  • Understanding of Quantum Field Theory concepts
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  • Knowledge of analytic continuation techniques
  • Basic grasp of Gamma functions and their properties
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  • Study the principles of dimensional regularization in Quantum Field Theory
  • Learn about analytic continuation and its applications in complex analysis
  • Explore the properties and applications of the Gamma function
  • Investigate specific examples of integrals evaluated using dimensional regularization
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Physicists, mathematicians, and students engaged in Quantum Field Theory, particularly those focusing on regularization techniques and integral evaluation methods.

mhill
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how does dimensional regularization work ?

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

[tex]\int d^{d} k F( \vec k )[/tex] ??

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

[tex]\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}[/tex]

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

[tex]\int_0^\infty dx\,{x^n\over x^2+1}.[/tex]

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

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

We now define this to be the value of the integral for all [itex]n[/itex].
 

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