What is the purpose of the exp[-(t^2)/2] term in Fourier transforms?

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The discussion centers on understanding the role of the exp[-(t^2)/2] term in Fourier transforms, particularly in the context of wave functions. This term is recognized as a localization factor that modifies the plane wave exp(i*w*t) to prevent it from being a pure plane wave. Participants emphasize the importance of comprehending Fourier series as a foundational step before tackling Fourier transforms. There is confusion over whether to take the Fourier transform of the entire function f(t) or just the localization term. Overall, a deeper understanding of these concepts is necessary for effective application in practical scenarios.
cytochrome
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I need more help understanding Fourier Transforms. I know that they transform a function from the time domain to the frequency domain and vice versa, but the short cuts to solve them just straight up confuse me.

http://www.cse.unr.edu/~bebis/CS474/Handouts/FT_Pairs1.pdf

This list of relations makes sense, but it's so hard for me to apply this to actual functions for some reason... I'd almost rather just do the integrals.

For example, every wave is of the form (except for the first exponential, which can always be different)

f(t) = exp[-(t^2)/2]exp(i*w*t)

The exp(i*w*t) part is the plane wave, correct? What is exp[-(t^2)/2] called? This term localizes the wave to keep it from being a plane wave, but I don't know what to call it.

Do you take the Fourier transform of the whole f(t), or just the localizing term?

Can someone please help me clear this up?
 
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cytochrome said:
For example, every wave is of the form (except for the first exponential, which can always be different)

f(t) = exp[-(t^2)/2]exp(i*w*t)


The exp(i*w*t) part is the plane wave, correct? What is exp[-(t^2)/2] called? This term localizes the wave to keep it from being a plane wave, but I don't know what to call it.

Where are you getting this part from? I suspect you are misunderstanding something with this. Fourier transforms allow us to decompose a function into contributions of individual waves of the form

F(\omega)e^{i\omega t}

F(\omega) can be any function (well, practically any). A given function f(t) determines F(\omega) and vice versa.

If you want to truly understand Fourier transforms, I recommend getting a good grasp of Fourier series first.
 
So I know that electrons are fundamental, there's no 'material' that makes them up, it's like talking about a colour itself rather than a car or a flower. Now protons and neutrons and quarks and whatever other stuff is there fundamentally, I want someone to kind of teach me these, I have a lot of questions that books might not give the answer in the way I understand. Thanks

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