I am looking to prove the functional equation for theta function. Source: https://www.youtube.com/watch?v=-GQFljOVZ7I&list=PL32446FDD4DA932C9&index=12 Time about 8.00. We are to integrate: $$\int_{-\infty+\frac{ik}{x}}^{+\infty+\frac{ik}{x}}e^{-\pi xz^2}dz$$ The argument is to change the bounds to $-\infty$ and $+\infty$ using something called Estimation Lemma or "ML-Inequality". I have absolutely no knowledge of complex analysis and integrals with complex variables. I've read in the comments, that one could say that $\infty+k = \infty $ for any finite number $k$, equivallently for $-\infty$ but as there is $i$, this argument seems invalid to me. Would anyone give me some deeper explanation of what we have actually done?
Improper definite integration with complex bounds
525 Views Asked by Bumbble Comm https://math.techqa.club/user/bumbble-comm/detail AtThere are 2 best solutions below
On
This is not an answer.
I am just showing that the naïve substitution $u=z-ik/x$ produces the correct answer to this integral with arbitrary real limits $a$ and $b$. Symmetry between the two limits is not leading to error cancellation in this case.
$$I=\int_{a+ik/x}^{b+ik/x} e^{-\pi x z^2}\,dz=\frac{\text{erf}\left(\frac{\sqrt{\pi } (b x+\text{ik})}{\sqrt{x}}\right)-\text{erf}\left(\frac{\sqrt{\pi } (a x+\text{ik})}{\sqrt{x}}\right)}{2 \sqrt{x}}$$
Using the substitution $u=z-ik/x$ gives
$$I=\int_{a}^{b} e^{-\pi x (u+ik/x)^2}\,du=\frac{\text{erf}\left(\frac{\sqrt{\pi } (b x+\text{ik})}{\sqrt{x}}\right)-\text{erf}\left(\frac{\sqrt{\pi } (a x+\text{ik})}{\sqrt{x}}\right)}{2 \sqrt{x}}$$
where erf is the error function
I am just curious as to why in this case this naïve substitution works for all real values of the limits $a$ and $b$.
In the video referenced in the OP, the narrator uses Cauchy's Integral Theorem to write
$$\int_{-R+ik/x}^{R+ik/x} e^{-\pi x z^2}\,dz=\int_{-R+ik/x}^{-R} e^{-\pi x z^2}\,dz+\int_{-R}^{R} e^{-\pi x z^2}\,dz+\int_{R}^{R+ik/x} e^{-\pi x z^2}\,dz\tag1$$
We can easily show that both the first and third integrals on the right-hand side of $(1)$ approach $0$ as $R\to \infty$. To do so, we assume without loss of generality that $k/x>0$ and develop bounds for the first integral on the right-hand side of $(1)$. Proceeding we find
$$\begin{align} \left|\int_{-R+ik/x}^{-R} e^{-\pi x z^2}\,dz\right|&\overbrace{=}^{z=-R+it} \left|\int_{k/x}^{0} e^{-\pi x (R-it)^2}\,i\,dt\right|\\\\ &\le \int_{0}^{k/x} \left| e^{-\pi x (R-it)^2}\,i\right|\,dt\\\\ &=\int_{0}^{k/x} \left| e^{-\pi x (R^2-t^2)}e^{i2\pi xRt}\,i\right|\,dt\\\\ &=\int_{0}^{k/x} e^{-\pi x (R^2-t^2)}\,dt\\\\ &\le \frac kx\,e^{-\pi x (R^2-(k/x)^2)}\tag2 \end{align}$$
As $R\to \infty$, the right-hand side of $(2)$ approaches $0$.
In an analogous development, we find that the third integral on the right-hand side of $(2)$ vanishes as $R\to \infty$ also.
Hence, we have
$$\lim_{R\to \infty}\int_{-R+ik/x}^{R+ik/x} e^{-\pi x z^2}\,dz=\lim_{R\to\infty}\int_{-R}^{R} e^{-\pi x z^2}\,dz=\frac{1}{\sqrt x}$$
And we are done!