576 C H A P T E R 10: Fourier Analysis of Discrete-Time Signals and Systems
a sinusoidx[n]=cos(ω 0 n+θ), which is not absolutely summable. According to the above pairs,
we getx[n]=1
2
[
ej(ω^0 n+θ)+e−j(ω^0 n+θ)]
⇔X(ejω)=π[
ejθδ(ω−ω 0 )+e−jθδ(ω+ω 0 )]
The DTFT of the cosine indicates that its power is concentrated at the frequencyω 0.The “dual” pairsδ[n−k], integerk⇔e−jωk (10.10)e−jω^0 n, −π≤ω 0 < π⇔ 2 πδ(ω+ω 0 ) (10.11)allow us to obtain the DTFT of signals that do not satisfy the absolutely summable condition. Thus, in general,
we have
∑kX[k]e−jωkn⇔∑k2 πX[k]δ(ω+ωk) (10.12)The linearity of the DTFT and the above result give that for a signal that is not absolutely summablex[n]=∑`A`cos(ω`n+θ`)its DTFT is
X(ejω)=∑`πA`[
ejθ`δ(ω−ω`)+e−jθ`δ(ω+ω`)]
−π≤ω < πIfx[n]is periodic, the discrete frequencies are harmonically related, i.e.,ω`=`ω 0 whereω 0 is the fundamental
frequency ofx[n].nExample 10.2
The DTFT of a signalx[n] isX(ejω)= 1 +δ(ω− 4 )+δ(ω+ 4 )+0.5δ(ω− 2 )+0.5δ(ω+ 2 )The signalx[n]=A+Bcos(ω 0 n)cos(ω 1 n)is given as a possible signal that givesX(ejω). Determine
whether you can findA,B, andω 0 andω 1 to obtain the desired DTFT. If not, provide a betterx[n].SolutionUsing trigonometric identities or Euler’s identity, we have thatcos(ω 0 n)cos(ω 1 n)=0.5 cos((ω 0 +ω 1 )n)+0.5 cos((ω 1 −ω 0 )n)