My goal is to evaluate ∫∞0dx1+xn(n∈N,n≥2).
Here is my approach:
Clearly, the integral converges.
Denote the value of the integral by In.
Now let γR describe the section of a circle which goes from the origin to R to Re2πi/n and back to the origin.
If we let CR denote the relevant circular arc, then
|∫CRdz1+zn|≤(2πRn)(1Rn−1)→0asR→∞.
Furthermore, ∫[R,Re2πi/n]dz1+zn=∫0Re2πi/ndr1+rn.
Hence lim
Thus if we can obtain the value of \int_{\gamma_R}\frac{dz}{1+z^n} we can evaluate I_n.
Now the zeroes of 1+z^n are of the form z=e^{i\pi/n+2\pi i m/n}\;\;(m\in\mathbb{N}) from which it is clear that the only zero which lies within the contour occurs at z=e^{i\pi/n} with multiplicity 1.
So all that remains to be done is to evaluate the residue of \frac{1}{1+z^n} at z=e^{i\pi/n}.
However, if z=e^{i\pi/n}u and u\neq1, we have
\frac{z^n+1}{z-e^{i\pi/n}}=\frac{1-u^n}{-e^{i\pi/n}(1-u)} =-e^{-i\pi/n}\sum_{m=0}^{n-1}u^m\;\;\;(2).
In particular, (2) implies Res_{z=e^{i\pi/n}}\frac{1}{1+z^n}=-\frac{e^{i\pi/n}}{n}\;\;\;(3).
Finally, (1) and (3) imply
I_n=\frac{2\pi i (Res_{z=e^{i\pi/n}}\frac{1}{1+z^n})}{1-e^{2\pi i/n}}=\frac{-2\pi ie^{i\pi/n}}{n(1-e^{2\pi i/n})}=\frac{\pi/n}{\sin(\pi/n)}.
I have three questions:
One, is my method correct?
Two, is there a simpler/different method to evaluate the integral?
Three, is there an easier way to evaluate the residue of \frac{1}{1+z^4} at z=e^{i\pi/n}?
Answer
Here is a different way. Lets more generally find the Mellin Transform.
Consider I(\alpha,\beta)=\int_{0}^{\infty}\frac{u^{\alpha-1}}{1+u^{\beta}}du=\mathcal{M}\left(\frac{1}{1+u^{\beta}}\right)(\alpha) Let x=1+u^{\beta} so that u=(x-1)^{\frac{1}{\beta}}. Then we have I(\alpha,\beta)=\frac{1}{\beta}\int_{1}^{\infty}\frac{(x-1)^{\frac{\alpha-1}{\beta}}}{x}(x-1)^{\frac{1}{\beta}-1}dx. Setting x=\frac{1}{v} we obtain I(\alpha,\beta)=\frac{1}{\beta}\int_{0}^{1}v^{-\frac{\alpha}{\beta}}(1-v)^{\frac{\alpha}{\beta}-1}dv=\frac{1}{\beta}\text{B}\left(-\frac{\alpha}{\beta}+1,\ \frac{\alpha}{\beta}\right).
Using the properties of the Beta and Gamma functions, this equals \frac{1}{\beta}\frac{\Gamma\left(1-\frac{\alpha}{\beta}\right)\Gamma\left(\frac{\alpha}{\beta}\right)}{\Gamma(1)}=\frac{\pi}{\beta\sin\left(\frac{\pi\alpha}{\beta}\right)}.
Your question is the case where \alpha =1.
Also see Chandru's answer on a different thread. It is another nice solution, along the lines of what you did above. (See this previous question, where both solutions can be found)
Hope that helps,
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