Along with examples of nonstationary processes, it is necessary to know a couple of examples of stationary processes.
Example 1. In the model with a time trend, suppose that there is no time trend, that is, $latex b=0$. The result is white noise shifted by a constant $latex a$, and it is seen to be stationary.
Example 2. Let us change the random walk slightly, by introducing a coefficient $latex \beta$ for the first lag:
(1) $latex y_t=\beta y_{t-1}+u_t$
where $latex u_t$ is, as before, white noise:
(2) $latex Eu_t=0$, $latex Eu_t^2=\sigma^2$ for all $latex t$ and $latex Eu_tu_s=0$ for all $latex t\ne s.$
This is an autoregressive process of order 1, denoted AR(1).
Stability condition. $latex |\beta|<1$.
By now you should be familiar with recurrent substitution. (1) for the previous period looks like this:
(3) $latex y_{t-1}=\beta y_{t-2}+u_{t-1}.$
Plugging (3) in (1) we get $latex y_t=\beta^2y_{t-2}+\beta u_{t-1}+u_t.$ After doing this $latex k$ times we obtain
(4) $latex y_t=\beta^ky_{t-k}+\beta^{k-1}u_{t-k+1}+...+\beta u_{t-1}+u_t.$
To avoid errors in calculations like this, note that in the product $latex \beta^{k-1}u_{t-k+1}$ the sum of the power of $latex \beta$ and the subscript of $latex u$ is always $latex t$.
Here the range of time moments didn't matter because the model wasn't dynamic. In the other example we had to assume that in (1) $latex t$ takes all positive integer values. In the current situation we have to assume that $latex t$ takes all integer values, or, put it differently, the process $latex y_t$ extends infinitely to plus and minus infinity. Then we can take advantage of the stability condition. Letting $latex k\rightarrow\infty$ (and therefore $latex t-k\rightarrow-\infty$) we see that the first term on the right-hand side of (4) tends to zero and the sum becomes infinite:
(5) $latex y_t=...+\beta^{k-1}u_{t-k+1}+...+\beta u_{t-1}+u_t=\sum_{j=0}^\infty\beta^ju_{t-j}.$
We have shown that this representation follows from (1). Conversely, one can show that (5) implies (1). (5) is an infinite moving average, denoted MA($latex \infty$).
It can be used to check that (1) is stationary. Obviously, the first condition of a stationary process is satisfied: $latex Ey_t=0$. For the second one we have (use (2)):
(6) $latex Var(y_t)=Ey_t^2=E(...+\beta^{k-1}u_{t-k+1}+...+\beta u_{t-1}+u_t)(...+\beta^{k-1}u_{t-k+1}+...+\beta u_{t-1}+u_t)$
$latex =...+\beta^{2k-2}Eu^2_{t-k+1}+...+\beta^2Eu^2_{t-1}+Eu^2_t=(...+\beta^{2k-2}+...+\beta^2+1)\sigma^2=\frac{\sigma^2}{1-\beta^2},$
which doesn't depend on $latex t$.
Exercise. To make sure that you understand (6), similarly prove that
(7) $latex Cov(y_t,y_s)=\beta^{|t-s|}\frac{\sigma^2}{1-\beta^2}.$
Without loss of generality, you can assume that $latex t>s$. (7) is a function of the distance in time between $latex t,s$, as required.
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