Periodicity of transfer function of FIR filter proof (Parks and Burrus, Digital Filter Design) In Digital Filter Design by Parks and Burrus, p. 19.



The transfer function of an FIR filter is given by the $\mathcal Z$-transform of $h(n)$ as:

$$H(z)=\sum_{n=0}^{N-1}h(n)z^{-n}$$

(where $h$ is the filter)

The frequency response of a filter is defined as

$$H(\omega)=\sum_{n=0}^{N-1} h(n)e^{-j\omega n}$$

where $\omega$ is frequency in $\textrm{rad/sec}$.

Then the text proceeds to show that $H(\omega)$ is periodic with period $2\pi$:

\begin{align}
H(\omega + 2 \pi)&amp;= \sum_{n=0}^{N-1} h(n) e^{-j(\omega+2\pi)n}\\
&amp;= \sum_{n=0}^{N-1} h(n) e^{- j \omega n} \color{red}{e^{-j2\pi n}}\\
&amp;=H(\omega)
\end{align}
Could someone clarify how is that equal to $H(\omega)$ when there's the extra term $\color{red}{e^{-j2 \pi n}}$?
$$\sum_{n=0}^{N-1}h(n)e^{-j\omega n}e^{-j2\pi n}=\sum_{n=0}^{N-1}h(n)e^{-j\omega n}\cdot1$$

Since
\begin{align}
e^{-j2\pi n}&amp;=\cos(-2\pi n) + j\sin(-2\pi n)\\
&amp;=\cos(2\pi n) - j\sin(2\pi n)\\
&amp;=1-0\\
&amp;=1
\end{align}