# Defining the Fourier Transform on LCA Groups

# Defining the Fourier Transform on LCA Groups

### We've already discussed how all of the variations on Fourier transforms can be unified in a single theory. But we didn't discuss how... until now!

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Join For FreeMy previous post said that all the familiar variations on Fourier transforms — Fourier series analysis and synthesis, Fourier transforms on the real line, discrete Fourier transforms, etc. — can be unified into a single theory. They're all instances of a Fourier transform on a locally compact Abelian (LCA) group. The difference between them is the underlying group.

Given an LCA group *G*, the Fourier transform takes a function on *G* and returns a function on the dual group of *G*. We said this much last time, but we didn't define the dual group; we just stated examples. We also didn't say just how you define a Fourier transform in this general setting.

## Characters and Dual Groups

Before we can define a dual group, we have to define group homomorphisms. A homomorphism between two groups *G* and *H* is a function *h* between the groups that preserves the group structure. Suppose the group operation is denoted by addition on *G* and by multiplication on *H* (as it will be in our application), saying *h* preserves the group structure means

Next, let *T* be the unit circle, i.e. complex numbers with absolute value 1. *T* is a group with respect to multiplication. (Why *T* for circle? This is a common notation, anticipating generalization to toruses in all dimensions. A circle is a one-dimensional torus.)

Now a character on *G* is a continuous homomorphism from *G* to *T*. The set of all characters on *G* is the dual group of *G*. Call this group *Γ*. If *G* is an LCA group, then so is *Γ*.

## Integration

The classical Fourier transform is defined by an integral. To define the Fourier transform on a group we have to have a way to do integration on that group. And there's a theorem that says we can always do that. For every LCA group, there exists a Haar measure *μ*, and this measure is nice enough to develop our theory. This measure is essentially unique: Any two Haar measures on the same LCA group must be proportional to each other. In other words, the measure is unique up to multiplying by a constant.

On a discrete group-for our purposes, think of the integers and the integers mod *m* -Haar measure is just counting; the measure of a set is the number of things in the set. And integration with respect to this measure is summation.

## Fourier Transform Defined

Let *f* be a function in *L*¹( *G*), i.e. an absolutely integrable function on *G*. Then the Fourier transform of *f* is a function on Γ defined by:

What does this have to do with the classical Fourier transform? The classical Fourier transform takes a function of time and returns a function of frequency. The correspondence between the classical Fourier transform and the abstract Fourier transform is to associate the frequency ω with the character that takes *x* to the value *exp( iω x)*.

There are multiple slightly different conventions for the classical Fourier transform cataloged here. These correspond to different constant multiples in the choice of measure on *G* and *Γ*, i.e. whether to divide by or multiply by √(2π), and in the correspondence between frequencies and characters, whether ω corresponds to exp(± *i*ω *x*) or exp(±2π *i*ω *x*).

Published at DZone with permission of John Cook , DZone MVB. See the original article here.

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