The idea behind Fourier series is to try and express some function on a domain [−L,L] into a sum of complex exponentials of the form 1√2Le2πi nx/L. One of the reasons this is interesting is that the complex exponentials are orthonormal system under the dot product ∫f(x)¯g(x) dx.
One can start by considering the vector space V of all square-integrable functions on [−L,L] -- this gives us a vector space with an inner product. Specifically, we're interested in the subspace Vn that is the span of complex exponentials upto n and −n.Then given a vector f in V, we can ask for its projection fn onto Vn.
As the complex exponentials are already orthonormal, it is easy to calculate this projection in their basis:
ak=⟨f,1√2Le2πinx/L⟩=L∫−Lf(x)e−2πikx/L√2Ldxfn(x)=∑|k|≤nake2πikx/L√2L
Notably this implies by Cauchy-Schwarz that:
|f|2⩾∑|k|⩽n|ak|2
This really just is Cauchy-Schwarz, and is known as Bessel's inequality. If we can show that the Fourier series approaches f, i.e. that ‖f−fn‖→0, then it would be obvious that
|f|2=∑|k|∈Z|ak|2
Which is just the Pythagoras theorem, and is known as Parseval's theorem. Obviously, these theorems exist in the general theory of Hilbert spaces.
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