The integral above can be expressed as , where and are rational numbers, find .
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With a > 0 , b > 0 consider
∫ 0 ∞ e − a x 2 sin ( b x 2 ) d x
We do contour integration. Let A = a 2 + b 2 .
Consider a positively oriented circular sector contour Γ of radius R with angle ω , which we define as follows. Note that there exists a unique 0 < θ < π / 2 such that
cos ( θ ) = a / A , sin ( θ ) = b / A
Let ω = θ / 2 .
Hence
cos ( ω ) = cos ( θ / 2 ) = 2 1 + a / A
and we can compute sin ( θ ) similarly.
Integrate f ( z ) = e − A z 2 over the contour. Note that this integral is 0 by Cauchy's Theorem.
Along the x-axis, the integral approaches
∫ 0 ∞ e − A x 2 d x = 2 A π
We can parametrize the circular part as z = R e i t for t from 0 to ω . So the integral along the circular part is
as R approaches infinity, since A > 0 and 4 π > ω .
Finally, parametrize the integral along the radial part by z = e i ω t for t from R to 0. We get
Edit: The above equation should not start with 0 but rather − 2 A π .
Using the above formulas for cos ( ω ) , sin ( ω ) and taking real and imaginary part, we have a system of equations and then can just solve for I1 and I2. I2 is what we want. Then just plug in the values for a and b and compute.
Anybody have a different/simpler solution?
Also, can we generalize this to not just involving x 2 but rather x n (I think so ...)?