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DTFT of (n+1)aⁿu[n]

Short answer

The signal can be expressed as a^n u[n] convolved with itself. DTFT of a^n u[n] is 1/(1−a e^{-jω}), so by convolution property X(e^{jω}) = 1/(1−a e^{-jω})^2.

Obtain the DTFT of the signal x[n] = (n+1)aⁿu[n], 0 < a < 1

Known pair: anu[n]↔11−ae−jωa^n u[n] \leftrightarrow \frac{1}{1-ae^{-j\omega}}, for ∣a∣<1|a|<1.

Property used (differentiation in frequency): n x[n]↔jdX(ejω)dωn\,x[n] \leftrightarrow j\frac{dX(e^{j\omega})}{d\omega}.

Step 1: split the signal.

x[n]=(n+1)anu[n]=n anu[n]+anu[n]x[n] = (n+1)a^n u[n] = n\,a^n u[n] + a^n u[n]

Step 2: DTFT of nanu[n]n a^n u[n].

jddω[11−ae−jω]=j⋅−(ja e−jω)(1−ae−jω)2=a e−jω(1−ae−jω)2\begin{aligned} j\frac{d}{d\omega}\left[\frac{1}{1-ae^{-j\omega}}\right] &= j\cdot\frac{-\left(ja\,e^{-j\omega}\right)}{(1-ae^{-j\omega})^2} \\ &= \frac{a\,e^{-j\omega}}{(1-ae^{-j\omega})^2} \end{aligned}

(derivative of 1−ae−jω1 - ae^{-j\omega} is ja e−jωja\,e^{-j\omega}).

Step 3: add the two parts.

X(ejω)=ae−jω(1−ae−jω)2+11−ae−jω=ae−jω+1−ae−jω(1−ae−jω)2=1(1−ae−jω)2\begin{aligned} X(e^{j\omega}) &= \frac{ae^{-j\omega}}{(1-ae^{-j\omega})^2} + \frac{1}{1-ae^{-j\omega}} \\ &= \frac{ae^{-j\omega} + 1 - ae^{-j\omega}}{(1-ae^{-j\omega})^2} \\ &= \frac{1}{(1-ae^{-j\omega})^2} \end{aligned}

Answer:

(n+1)anu[n]  ⟷  1(1−ae−jω)2,0<a<1(n+1)a^n u[n] \;\longleftrightarrow\; \frac{1}{\left(1 - a e^{-j\omega}\right)^2}, \quad 0<a<1

Check by convolution: (n+1)anu[n]=anu[n]∗anu[n](n+1)a^n u[n] = a^n u[n] * a^n u[n], since ∑k=0nakan−k=(n+1)an\sum_{k=0}^{n}a^k a^{n-k} = (n+1)a^n. Convolution in time gives the product 11−ae−jω⋅11−ae−jω\frac{1}{1-ae^{-j\omega}}\cdot\frac{1}{1-ae^{-j\omega}}, the same result.

Magnitude: ∣X(ejω)∣=11−2acos⁡ω+a2|X(e^{j\omega})| = \frac{1}{1 - 2a\cos\omega + a^2}, maximum 1(1−a)2\frac{1}{(1-a)^2} at ω=0\omega = 0. Phase: −2tan⁡−1asin⁡ω1−acos⁡ω-2\tan^{-1}\frac{a\sin\omega}{1-a\cos\omega}.

✓ Answer checked by Claude Opus 5.5 (high effort)

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