As part of a recent question I posted, I decided to try and generalise for a power of 2 to any r∈R. As part of the method I took, I had to solve the following integral:
I=∫∞011+xrdx
I believe what I've done is correct, but I'm concerned that I may missed something (in particular whether it holds for all r≠0). So, here I have two questions (1) Is what I've done correct? and (2) What other methods can be employed that doesn't rely on complex analysis?
Here is the method I took:
First make the substitution u=x1r to arrive at
I=1n∫∞011+u⋅u1−1rdu
We now substitute t=11+u to arrive at:
I=1r∫01t⋅(1−tt)1r−11t2dt=1r∫10t−1r(1−t)1r−1dt=1rB(1−1n,1+1r−1)=1rB(r−1r,1r)=1rB(r−1r,1r)
Wheer B(a,b) is the Beta function. Using the relationship between the Beta and Gamma function we arrive at:
I=1rΓ(r−1r)Γ(1r)Γ(r−1r+1r)=1rΓ(r−1r)Γ(1r)
And so, we arrive at:
I=∫∞011+xrdx=1rΓ(r−1r)Γ(1r)
for r>1
As per KemonoChen's comment and others, we can employ Euler's Reflection Formula to position this result for 1r∉Z Here, as r∈R,r>1→1r∉Z and so our formula holds.
I=∫∞011+xrdx=1rΓ(r−1r)Γ(1r)=πrsin(πr)
Thank you also to Winther, Jjagmath, and MrTaurho's for their comments and corrections/clarifications.
Answer
Your given integral is closely related to the Mellin transform and can be evaluated by using Ramanujan's Master Theorem.
Ramanujan's Master Theorem
Let f(x) be an analytic function with a MacLaurin Expansion of the form
f(x)=∞∑k=0ϕ(k)k!(−x)kthen the Mellin Transform of this function is given by
∫∞0xs−1f(x)dx=Γ(s)ϕ(−s)
In order to get there we can expand the fraction as a geometric series
I=∫∞011+xndx=∫∞0∞∑k=0(−1)kxkndx
Now by applying the substitution t=xn followed by a little bit of reshaping yields to
I=∫∞0∞∑k=0(−1)kxkndx=1n∫∞0t1/n−1∞∑k=0(−1)kk!k!tkdt=1n∫∞0t1/n−1∞∑k=0(−1)kϕ(k)k!tkdt
Now we can apply Ramanujan's Master Theorem with s=1/n and ϕ(k)=Γ(k+1) to get
I=1n∫∞0t1/n−1∞∑k=0(−1)kϕ(k)k!tkdt=1nΓ(1n)Γ(1−1n)
And finally this can be simplified, as already pointed out, by using Euler's Reflection Formula (as long as it holds i.e. for all 1/n∉Z) to get
I=∫∞011+xndx=1nπsin(πn)
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