Let's restrict this discussion to those stretched exponentials in the article you linked to, since they have the property that their limit is zero as $t \to +\infty$, which makes talking about the concept of "falling" relatively straightforward.
If we have two such functions, $f$ and $g$, then to say "$g$ falls more slowly than $f$" means that $g$ approaches $0$ more slowly than $f$ does. In other words, $f$ falls (decreases) more quickly than $g$ does. So it is the case that $\displaystyle\lim_{t\to +\infty} \frac{f(t)}{g(t)} = 0$, because the numerator approaches $0$ more quickly than the denominator does. There are two ways of stating this here:
$$ \lim_{t \to+\infty} \frac{f(t)}{g(t)} = 0 \qquad \text{and} \qquad \lim_{t\to+\infty} \frac{g(t)}{f(t)} = +\infty$$
In general, $g(t) = e^{-t^\beta}$ falls more slowly than $f(t) = e^{-t}$ if we have $\beta < 1$. That's just from the link you provided. Consider:
$$ \lim_{t\to +\infty} \frac{g(t)}{f(t)} = \lim_{t\to +\infty} \frac{e^{-t^\beta}}{e^{-t}} = \lim_{t\to+\infty} \frac{e^{-t^\beta} \cdot e^t}{e^{-t} \cdot e^t} = \lim_{t\to+\infty} e^{t-t^\beta}$$
Since $\beta < 1$ and $t \to +\infty$, then $t^\beta \to 0$. Thus $t - t^\beta \to +\infty$ as $t \to +\infty$, and so $\displaystyle \lim_{t\to+\infty} e^{t-t^\beta} = +\infty$. This paragraph isn't exactly rigorous, but I'm going for clarity here.
A similar argument shows the other limit mentioned above: $\displaystyle\lim_{t\to+\infty} \frac{f(t)}{g(t)} = 0$