Summation of exponential terms

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The discussion centers on proving an identity involving the summation of exponential terms, specifically relating to the transformation of the variable α. The identity presented shows a connection between two sums, suggesting they are scaled versions of each other. Participants explore the implications of changing α to αβ and how this affects the sums, noting that both can be approximated as Gaussian integrals. Concerns are raised about the normalization factor when transitioning from summation to integral. A question is posed regarding whether α must be a positive integer for the identity to hold.
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I found the following identity in a paper:
##
\sum_{l=1}^{\infty}exp(-\pi\alpha l^2)=(\frac{1}{2\sqrt{\alpha}}-\frac{1}{2})+\frac{1}{\sqrt{\alpha}}\sum_{l=1}^{\infty}exp(\frac{-\pi l^2}{\alpha}) ##
Someone please let me give some hints on how to prove this.
 
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It looks like it's the same sum on both sides, but scaled.

I would see what happens to the exponential sum when you change \alpha to \alpha\beta. Can you make the result identical with the right scaling factor in front (twice as wide, but half as tall)?
 
Yes, it's the same sum but scaled. One thing I have found that if you approximate the summation as integral, it can be proved easily as both are usual Gaussian Integral. But I was worrying about the factor that involves to transform the summation into integral. Any thoughts?
 
So, you can write it alternatively as:
\frac{1}{2} +\sum_{l=1}^{\infty}exp(-\pi\alpha l^2)=\frac{1}{\sqrt{\alpha}}\big(\frac{1}{2}+\sum_{l=1}^{\infty}exp(\frac{-\pi l^2}{\alpha})\big)
or better yet
\sum_{l=-\infty}^{\infty}exp(-\pi\alpha l^2)=\frac{1}{\sqrt{\alpha}}\sum_{l=-\infty}^{\infty}exp(\frac{-\pi l^2}{\alpha})
this sum is exactly the integral of a discrete gaussian. With the normalization constant in front, they should have the same area..

At least, that is how I think it should work out.

Does \alpha have to be a positive integer?
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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