Undergrad Can a Gaussian distribution be represented as a sum of Dirac Deltas?

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A Dirac Delta function can be approximated as a limiting case of a Gaussian distribution as the width approaches zero. Conversely, it is proposed that a Gaussian spectrum can be represented as a weighted sum of Dirac Deltas, where the weights determine the distribution. While any function can be expressed as an integral of Dirac delta functions, a discrete sum representation is not feasible for most functions. However, an approximation using small increments can be made, allowing for a representation that works in an integration sense. This discussion highlights the relationship between Gaussian distributions and Dirac delta functions in mathematical modeling.
tworitdash
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We know that Dirac Delta is not a function. However, I just talk about the numerical version of it that we use every day. We can simply represent the Dirac delta function as a limiting case of Gaussian distribution when the width of the distribution ##\sigma->0##.

$$
\delta(x - \mu) = lim_{\sigma -> 0} \frac{1}{\sqrt{2\pi \sigma^2}} e^{\frac{-(x - \mu)^2}{2\sigma^2}}
$$

Is it possible to also say the reverse with a weighted sum of Dirac Deltas to construct a Gaussian spectrum?

$$
\frac{1}{\sqrt{2\pi \sigma^2}} e^{\frac{-(x - mu)^2}{2\sigma^2}} = \sum_{i} w_i \delta(x - i)
$$

Where, somehow the weights ##w_i## constitute how it is distributed (##\sigma##). If yes, how do we decide these weights?
 
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Any function can be represented as a sum of Dirac delta functions:

Let ##f(x)## be an arbitrary function of ##x##. Then you can represent it as:

##\int f(y) \delta(x-y) dy##

So that's a weighted sum (well, integral) of delta functions.
 
stevendaryl said:
Any function can be represented as a sum of Dirac delta functions:

Let ##f(x)## be an arbitrary function of ##x##. Then you can represent it as:

##\int f(y) \delta(x-y) dy##

So that's a weighted sum (well, integral) of delta functions.

If you really want a discrete sum, instead of an integral, then it can't be done for most functions. But I guess for some purposes, you can approximate a function by delta functions: Pick a small positive x increment ##\Delta x## and define ##\tilde{f}(x, \Delta x)## by:

##\tilde{f}(x, \Delta x) = \sum_j f(j \Delta x) \delta(x- j\Delta x) \Delta x##

where ##\Delta x## is some small real number. This approximation works in an integration sense: For any other smooth function ##g(x)##, we have:

##lim_{\Delta x \Rightarrow 0} \int \tilde{f}(x, \Delta x) g(x) dx = \int f(x) g(x) dx##
 
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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