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Discrete Time Complex Exponential

Module by: Dan Calderon, Richard Baraniuk, Stephen Kruzick. E-mail the authors

Based on: The Complex Exponential by Richard Baraniuk

Summary: Describes the complex exponential function for discrete time.

Introduction

Complex exponentials are some of the most important functions in our study of signals and systems. Their importance stems from their status as eigenfunctions of linear time invariant systems. Before proceeding, you should be familiar with complex numbers.

The Discrete Time Complex Exponential

Complex Exponentials

The complex exponential function will become a critical part of your study of signals and systems. Its general discrete form is written as

A⁢es⁢n A s n
(1)
where s=σ+j⁢ω s σ ω , is a complex number in terms of σσ, the attenuation constant, and ωω the angular frequency.

The discrete time complex exponentials have the following property, which will become evident through discussion of Euler's formula.

ej⁢ω⁢n=ej⁢(ω+2⁢π)⁢n ω n ω 2 n
(2)
Given this property, if we have a complex exponential with frequency ω+2⁢π ω 2 , then this signal "aliases" to a complex exponential with frequency ωω, implying that the equation representations of discrete complex exponentials are not unique.

Euler's Formula

The mathematician Euler proved an important identity relating complex exponentials to trigonometric functions. Specifically, he discovered the eponymously named identity, Euler's formula, which states that

e j x = cos ( x ) + j sin ( x ) e j x = cos ( x ) + j sin ( x )
(3)

which can be proven as follows.

In order to prove Euler's formula, we start by evaluating the Taylor series for ezez about z=0z=0, which converges for all complex zz, at z=jxz=jx. The result is

e j x = ∑ k = 0 ∞ ( j x ) k k ! = ∑ k = 0 ∞ ( - 1 ) k x 2 k ( 2 k ) ! + j ∑ k = 0 ∞ ( - 1 ) k x 2 k + 1 ( 2 k + 1 ) ! = cos ( x ) + j sin ( x ) e j x = ∑ k = 0 ∞ ( j x ) k k ! = ∑ k = 0 ∞ ( - 1 ) k x 2 k ( 2 k ) ! + j ∑ k = 0 ∞ ( - 1 ) k x 2 k + 1 ( 2 k + 1 ) ! = cos ( x ) + j sin ( x )
(4)

because the second expression contains the Taylor series for cos(x)cos(x) and sin(x)sin(x) about t=0t=0, which converge for all real xx. Thus, the desired result is proven.

Choosing x=ωnx=ωn this gives the result

e j ω n = cos ( ω n ) + j sin ( ω n ) e j ω n = cos ( ω n ) + j sin ( ω n )
(5)

which breaks a discrete time complex exponential into its real part and imaginary part. Using this formula, we can also derive the following relationships.

cos ( ω n ) = 1 2 e j ω n + 1 2 e - j ω n cos ( ω n ) = 1 2 e j ω n + 1 2 e - j ω n
(6)
sin ( ω n ) = 1 2 j e j ω n - 1 2 j e - j ω n sin ( ω n ) = 1 2 j e j ω n - 1 2 j e - j ω n
(7)

Discrete Time Phasors

It has been shown how the complex exponential with purely imaginary frequency can be broken up into its real part and its imaginary part. Now consider a general complex frequency s=σ+ωjs=σ+ωj where σσ is the attenuation factor and ωω is the frequency. Also consider a phase difference θθ. It follows that

e ( σ + j ω ) n + j θ = e σ n cos ( ω n + θ ) + j sin ( ω n + θ ) . e ( σ + j ω ) n + j θ = e σ n cos ( ω n + θ ) + j sin ( ω n + θ ) .
(8)

Thus, the real and imaginary parts of esnesn appear below.

Re { e ( σ + j ω ) n + j θ } = e σ n cos ( ω n + θ ) Re { e ( σ + j ω ) n + j θ } = e σ n cos ( ω n + θ )
(9)
Im { e ( σ + j ω ) n + j θ } = e σ n sin ( ω n + θ ) Im { e ( σ + j ω ) n + j θ } = e σ n sin ( ω n + θ )
(10)

Using the real or imaginary parts of complex exponential to represent sinusoids with a phase delay multiplied by real exponential is often useful and is called attenuated phasor notation.

We can see that both the real part and the imaginary part have a sinusoid times a real exponential. We also know that sinusoids oscillate between one and negative one. From this it becomes apparent that the real and imaginary parts of the complex exponential will each oscillate within an envelope defined by the real exponential part.

Figure 1: The shapes possible for the real part of a complex exponential. Notice that the oscillations are the result of a cosine, as there is a local maximum at t=0 t 0 . Of course, these drawings would be sampled in a discrete time setting.
(a) If σσ is negative, we have the case of a decaying exponential window. (b) If σσ is positive, we have the case of a growing exponential window.(c) If σσ is zero, we have the case of a constant window.
Figure 1(a) (compexp1.png)Figure 1(b) (compexp2.png)Figure 1(c) (compexp3.png)

Discrete Complex Exponential Demonstration

Figure 2: Interact (when online) with a Mathematica CDF demonstrating the Discrete Time Complex Exponential. To Download, right-click and save target as .cdf.
ComplexExponentialDemo

Discrete Time Complex Exponential Summary

Discrete time complex exponentials are signals of great importance to the study of signals and systems. They can be related to sinusoids through Euler's formula, which identifies the real and imaginary parts of purely imaginary complex exponentials. Eulers formula reveals that, in general, the real and imaginary parts of complex exponentials are sinusoids multiplied by real exponentials. Thus, attenuated phasor notation is often useful in studying these signals.

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