3.1 Definition

Denote the summation in Eq. (33) by Hn:

     N∑−1      (  2π   )
Hn ≡     hjexp  − i--nj .
      j=0          N
(34)

Then Hn with n = 0,1,N 1 is called the Discrete Fourier transformation (DFT) of hj with j = 0,1,,N 1. (The efficient algorithm of computing the DFT is discussed in Appendix A.)

Why do we choose n to be in the positive range [0 : N 1]? This is to make the tranform pair symmetric: both j and n are in the same range. This symmetry is helpful in making the transform pair easy to remember. This does not mean we only need the positive frequency components. In fact, we usually need n in the range [N∕2,N∕2]. This will be discussed in the next section.

In terms of Hn, the Fourier expansion coefficients cn in Eq. (33) is written as

c = -1H  .
 n  N   n
(35)

The corresponding frequency is

fn = n-= -n--= fs n-.
     T   ΔN      N
(36)

Here f1 is called the fundamental frequency (spacing in the frequency domain).