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Fourier Transform

Question

How can every function be expressed as a sum of sine and cosine waves?

Some Setup

Imagine the R3\mathbb{R}^3. Any point in this space is accessable by projecting onto the basis directions. This vector space is not structured enough. We can not measure length, angle, and similarity.

A inner product is a function that maps two vectors to a number (scalar). It must be:

From this you can get: length (norm)

x=x,x\|x\| = \sqrt{\langle x,x \rangle}

Without positivity, vectors lengths could be imaginary length.

angle

cosθ=x,yxy\cos\theta = \frac{|\langle x,y\rangle|}{\|x\| \|y\|}

Without symmetry, angles become asymmetric.

Orthogonality

x,y=0⟨x,y⟩=0

Projection and general decomposition would fail.

In Hilbert space of functions, all elements are functions NOT vectors. A function is a point in an infinite-dimensional space. The inner product is the dot product. It measure how align two functions are.

f,g=f(t)g(t)dt\langle f, g \rangle = \int f(t) g(t) \, dt

Key Idea

A Fourier transform converst a signal over time into frequencies inside the signal.

f^(ω)=f(x)eiωxdx\hat{f}(\omega) = \int_{-\infty}^{\infty} f(x)e^{-i\omega x}\,dx

f(x)f(x) is the original signal and f^(ω)\hat{f}(\omega) is the frequency spectrum and ww is the frequency. Note that it’s the original function f(x)f(x) multipled against the term eiwx e^{-iwx}

Where does the term come from? eiθ=cos(θ)+isin(θ) e^{i\theta} = cos(\theta) + i sin(\theta)

Requirements

Absolute Integrability (L1L^1 condition)

The function must decay fast enough so the total area is finite.

Piecewise Continuity

The function must be piecewise continuous on finite intervals.

Dirichlet Conditions

Relaxed Conditions

To generalize it, you can define the transform using distributions

Why Bother?

Recasting a function or math object into another coordinate system is a common trick to solve problems that otherwise would not be easily solvable.


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