October 6 (Friday)
Topics:
Fourier inversion formula
Fourier Series for periodic function
Interpretation of complex vector space, hermitian inner product, orthonormal basis.
Suppose you started from f(x), and did some hard work to get the Fourier transformation F(p). Can you recover f(x) from F(p)? Did you lose information when you throw away f(x) and only keep F(p)?
If f(x) is continuous and absolutely integrable, we can recover f(x) from F(p) by
f(x)=2π1∫p∈RF(p)eipxdp
The proof of this theorem is beyond the scope of this class. You might be happy to just accept the formal 'rule' that
2π1∫Reipx−ipydp=δ(x−y).
and that
f(x)=∫δ(x−y)f(y)dy
We can try some example to see if it works.
Fourer Series
If the function f(x) is a periodic function, of period L, meaning f(x)=f(x+L), then we cannot do Fourier transform (why?), but instead, we need to do Fourier series.
We are not going to use all eipx for all p, but only those that satisfies eipx=eip(x+L) have the same periodicity. Which mean p needs to satisfy
p=(2π/L)n for some integer n.
So, we define
en(x)=ei(2π/L)nx.
We define the Fourer series coefficient as
cn=L1∫0Lf(x)en(x)dx
Given these coefficient cn, can we recover f(x)? Yes, under some smoothness condition of f(x), we have
f(x)=n∈Z∑cnen(x).