Let f(z)=e−z2/2 and γ=γ1+γ2+γ3+γ4 be this path, where a>0 and R>0.
I need to show that
∫∞0e−t2/2cos(at)dt=√π2e−a2/2.(∗)
The first part of the exercise was to show that
lim
I was able to do that. I can also use that f has a primitive. Because \gamma is closed it is also clear, that
\lim_{R\to\infty} \int_{\gamma_1} f(z)dz + \lim_{R\to\infty} \int_{\gamma_3} f(z)dz = 0.
I am unsure what to do next to solve the integral (*).
Answer
Let \gamma_{1} be the curve t for t\in [-R,R] and \gamma_{3} be the curve ia -t for t\in [-R,R].
Then
\lim_{R\rightarrow \infty}\int_{\gamma_{1}} f(z)\operatorname{d}\!z + \lim_{R\rightarrow\infty}\int_{\gamma_{2}} f(z) \operatorname{d}\!z = \lim_{R\rightarrow\infty} \int_{-R}^{R} e^{-t^{2}/2} - e^{-(ia-t)^{2}/2}\operatorname{d}\!t.
Now I'll leave it to you to calculate the LHS of
\operatorname{Re}\left[ \lim_{R\rightarrow\infty} \int_{-R}^{R} e^{-t^{2}/2} - e^{-(ia-t)^{2}/2}\operatorname{d}\!z\right] = 0
and proceed from there.
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