Advanced Z-Transform Properties: Conjugation, Accumulation, Correlation, and Parseval
The full property table beyond shifting and convolution, with ROC rules and proofs of accumulation and Parseval.
The Complete Property Table
Let
\[x[n]\;\xleftrightarrow{\;\mathcal{Z}\;}X(z),\quad \text{ROC}=R_x \qquad y[n]\;\xleftrightarrow{\;\mathcal{Z}\;}Y(z),\quad \text{ROC}=R_y\]| Property | Time domain | Z-domain | ROC |
|---|---|---|---|
| Linearity | $ax[n]+by[n]$ | $aX(z)+bY(z)$ | contains $R_x\cap R_y$ |
| Time shift | $x[n-n_0]$ | $z^{-n_0}X(z)$ | $R_x$ (minus $z=0$ or $\infty$) |
| Frequency shift | $e^{j\omega_0 n}x[n]$ | $X(e^{-j\omega_0}z)$ | $R_x$ |
| Exponential scaling | $a^n x[n]$ | $X(a^{-1}z)$ | $\vert a\vert R_x$ |
| Differentiation | $n\,x[n]$ | $-z\dfrac{dX(z)}{dz}$ | $R_x$ |
| Conjugation | $x^*[n]$ | $X^(z^)$ | $R_x$ |
| Reversal | $x[-n]$ | $X(1/z)$ | $1/R_x$ |
| Real part | $\operatorname{Re}{x[n]}$ | $\tfrac12[X(z)+X^(z^)]$ | $R_x$ |
| Imaginary part | $\operatorname{Im}{x[n]}$ | $\tfrac{1}{2j}[X(z)-X^(z^)]$ | $R_x$ |
| Convolution | $x[n]*y[n]$ | $X(z)Y(z)$ | contains $R_x\cap R_y$ |
| Correlation | $r_{xy}[n]=\sum_k x[k]y[k-n]$ | $X(z)Y(z^{-1})$ | contains $R_x\cap 1/R_y$ |
| Accumulation | $\sum_{k=-\infty}^{n}x[k]$ | $\dfrac{X(z)}{1-z^{-1}}$ | contains $R_x\cap{\vert z\vert>1}$ |
| Multiplication | $x[n]y[n]$ | $\dfrac{1}{2\pi j}\oint_C X(v)Y(z/v)v^{-1}dv$ | — |
| Parseval | $\sum_n x[n]y^*[n]$ | $\dfrac{1}{2\pi j}\oint_C X(z)Y^(1/z^)z^{-1}dz$ | — |
Conjugation and Its Consequences
\[x^*[n]\;\longleftrightarrow\;X^*(z^*),\qquad \text{ROC}=R_x\]Proof.
\[\sum_n x^*[n]z^{-n}=\left(\sum_n x[n](z^*)^{-n}\right)^*=X^*(z^*)\]What Conjugation Buys You
For a real sequence $x[n]=x^*[n]$, the property forces
\[X(z)=X^*(z^*)\]On the unit circle $z=e^{j\omega}$, $z^*=e^{-j\omega}$, so
\[X(e^{j\omega})=X^*(e^{-j\omega})\]This is conjugate symmetry of the DTFT of any real signal. Splitting into magnitude and phase:
\[\vert X(e^{j\omega})\vert=\vert X(e^{-j\omega})\vert \quad\text{(even)}\] \[\angle X(e^{j\omega})=-\angle X(e^{-j\omega}) \quad\text{(odd)}\]Consequences you use constantly:
- A real signal’s spectrum needs only $\omega\in[0,\pi]$; the negative half is redundant.
- The DFT of a real $N$-point sequence satisfies $X[N-k]=X^*[k]$.
- Real filters have real coefficients, so $H(e^{j\omega})$ is conjugate-symmetric — the phase is odd and the magnitude is even.
Real and Imaginary Parts
Decompose $x[n]=x_r[n]+jx_i[n]$. Then
\[x_r[n]=\tfrac12\left(x[n]+x^*[n]\right) \;\longleftrightarrow\; \tfrac12\left[X(z)+X^*(z^*)\right]\] \[x_i[n]=\tfrac{1}{2j}\left(x[n]-x^*[n]\right) \;\longleftrightarrow\; \tfrac{1}{2j}\left[X(z)-X^*(z^*)\right]\]These are just conjugation combined with linearity. They are useful when separating the response of a complex-valued system into its real and quadrature channels.
Time Reversal
\[x[-n]\;\longleftrightarrow\;X(1/z),\qquad \text{ROC}=1/R_x\]Proof: substitute $m=-n$:
\[\sum_n x[-n]z^{-n}=\sum_m x[m](z^{-1})^{-m}=X(z^{-1})\]The ROC inverts: if $R_x$ is $\vert z\vert>r$, the reversed signal’s ROC is $\vert z\vert<1/r$.
Practical use: reversing a sequence turns a causal filter into an anti-causal one, which is exactly how zero-phase filtering (filtfilt) works — filter forward, reverse, filter again, reverse back, so the phase distortions cancel.
Convolution and Correlation
Convolution:
\[y[n]=x[n]*y_0[n]=\sum_k x[k]\,y_0[n-k] \;\longleftrightarrow\; Y_0(z)=X(z)Y_0(z)\]Correlation (note the missing time reversal compared with convolution):
\[r_{xy}[n]=\sum_{k=-\infty}^{\infty}x[k]\,y[k-n] \;\longleftrightarrow\; R_{xy}(z)=X(z)Y(z^{-1})\]Proof. Let $m=k-n$, so $k=m+n$:
\[\sum_n r_{xy}[n]z^{-n}=\sum_n\sum_k x[k]y[k-n]z^{-n}=\sum_k x[k]z^{k}\sum_m y[m]z^{-m}\] \[=\left(\sum_k x[k](z^{-1})^{-k}\right)\left(\sum_m y[m]z^{-m}\right)=X(z^{-1})\,Y(z)\](equivalently $X(z)Y(z^{-1})$ by re-indexing). For the autocorrelation, $Y=X$:
\[r_{xx}[n]\;\longleftrightarrow\;X(z)X(z^{-1})\]On the unit circle this becomes $\vert X(e^{j\omega})\vert^2$ — the energy spectral density. That is the Z-domain statement of the Wiener–Khinchine theorem.
Accumulation
\[y[n]=\sum_{k=-\infty}^{n}x[k]\;\longleftrightarrow\;Y(z)=\frac{X(z)}{1-z^{-1}}\]Proof. Note $y[n]-y[n-1]=x[n]$. Transform both sides:
\[Y(z)-z^{-1}Y(z)=X(z)\;\Rightarrow\;Y(z)(1-z^{-1})=X(z)\]The ROC must contain both $R_x$ and $\vert z\vert>1$, because the accumulator has a pole at $z=1$. This is the discrete counterpart of integration ($1/s$ in the Laplace domain).
Example. $x[n]=\delta[n]$ accumulates to $u[n]$:
\[X(z)=1,\qquad Y(z)=\frac{1}{1-z^{-1}}=U(z) \;\checkmark\]Stability warning: the accumulator is marginally stable — its pole sits exactly on the unit circle at $z=1$. A bounded input like $u[n]$ produces an unbounded output, so the accumulator is not BIBO stable.
Parseval’s Relation
For two sequences:
\[\sum_{n=-\infty}^{\infty}x[n]\,y^*[n]=\frac{1}{2\pi j}\oint_C X(z)\,Y^*(1/z^*)\,z^{-1}\,dz\]For $y=x$ this is the energy theorem:
\[\sum_n \vert x[n]\vert^2=\frac{1}{2\pi j}\oint_C X(z)X^*(1/z^*)\,z^{-1}\,dz\]On the unit circle $z=e^{j\omega}$, $dz=j e^{j\omega}d\omega=jz\,d\omega$, so $z^{-1}dz=j\,d\omega$ and the contour integral collapses to
\[\boxed{\sum_n \vert x[n]\vert^2=\frac{1}{2\pi}\int_{-\pi}^{\pi}\vert X(e^{j\omega})\vert^2\,d\omega}\]Meaning: energy computed in time equals energy computed in frequency. No energy is lost or created by the transform; the transform only redistributes it.
Discrete (DFT) Version
\[\sum_{n=0}^{N-1}\vert x[n]\vert^2=\frac{1}{N}\sum_{k=0}^{N-1}\vert X[k]\vert^2\]This is the version you actually use numerically. It lets you compute signal energy from the FFT without ever reconstructing the time signal.
Worked ROC Problems
Example 1: Sum of Two Right-Sided Sequences
\[x[n]=\left(\tfrac12\right)^n u[n]+\left(\tfrac13\right)^n u[n]\]Poles at $z=\tfrac12$ and $z=\tfrac13$. Both are right-sided, so
\[X(z)=\frac{z}{z-\frac12}+\frac{z}{z-\frac13},\qquad \text{ROC: }\vert z\vert>\frac12\]The ROC is the intersection of the individual ROCs, bounded by the outermost pole.
Example 2: Right-Sided Plus Left-Sided
\[x[n]=\left(\tfrac12\right)^n u[n]-\left(\tfrac13\right)^n u[-n-1]\]First term: pole at $\tfrac12$, ROC $\vert z\vert>\tfrac12$. Second term: pole at $\tfrac13$, ROC $\vert z\vert<\tfrac13$.
\[X(z)=\frac{z}{z-\frac12}+\frac{z}{z-\tfrac13},\qquad \text{ROC: }\frac13<\vert z\vert<\frac12\]The intersection is empty unless the two sides do not overlap — here $\tfrac13<\tfrac12$, so the ROC is the annulus between the poles and is non-empty. If the second pole had been at $\tfrac23$, the intersection would be empty and no Z-transform would exist for that combination.
Example 3: Finite-Length Sequence
\[x[n]=\{1,\ 2,\ 3\},\quad n=0,1,2\] \[X(z)=1+2z^{-1}+3z^{-2}\]The ROC is the entire $z$-plane except $z=0$ (because of the $z^{-1}$ and $z^{-2}$ terms). A finite sequence has no poles, so nothing bounds its ROC.
Example 4: Does the DTFT Exist?
\[x[n]=2^n u[n]\] \[X(z)=\frac{z}{z-2},\qquad \text{ROC: }\vert z\vert>2\]The ROC does not include the unit circle $\vert z\vert=1$, so the DTFT does not exist — the sequence grows without bound. The Z-transform still exists as a formal object, which is precisely why the Z-transform is more general.
Property Cheat Sheet by Question Type
| Question asks | Property to reach for |
|---|---|
| “Effect of delaying by 3?” | $z^{-3}X(z)$ |
| “Effect of multiplying by $n$?” | $-z\,dX/dz$ |
| “Effect of reversing?” | $X(1/z)$, ROC inverts |
| “Is the DTFT real/even?” | Conjugation + real signal |
| “Relate convolution and correlation” | $X(z)Y(z)$ vs $X(z)Y(z^{-1})$ |
| “Energy in frequency domain” | Parseval |
| “Output of an accumulator” | $X(z)/(1-z^{-1})$ |
| “Where can the ROC be?” | Intersection of individual ROCs, never containing poles |