Consider the difference equations
$$x(k+1) = f(x(k)) \qquad (1)$$
and
$$y(k+1) = g(y(k)) \qquad (2)$$
where $g = f \circ f$.
In An Introduction to Difference Equations (3e) by Saber Elaydi, in the proof of Theorem 1.16 (on p.32), it is mentioned that for $a$ an equilibrium of (1), if $a$ is an asymptotically stable equilibrium of (2), then it is also an asymptotically stable equilibrium for (1).
How can we prove this?
My progress so far
- Since $g(x) = f(f(x))$,
- $g'(x) = f'(f(x))f'(x)$
- $g''(x) = f''(f(x)) [f'(x)]^2 + f'(f(x)) f''(x)$
- $g'''(x) = f'''(f(x)) f'(x) [f'(x)]^2 + 2f''(f(x)) f'(x) f''(x) + f''(f(x)) f'(x) f''(x) + f'(f(x))f'''(x)$
- Assume $a$ is an asymptotically stable equilibrium for (2). There are two cases
- $|g'(a)| < 1$
- $|g'(a)| = 1$, $g''(a) = 0$, and $g'''(a) < 0$
- Note that $g'(a) = f'(f(a))f'(a) = [f'(a)]^2$
- Hence when $|g'(a)| < 1$, $|f'(a)| < 1$ as well. In this case $a$ is an asymptotically stable equilibrium of (1)
- Now assume $|g'(a)| = 1$, $g''(a) = 0$, and $g'''(a) < 0$.
- Since $g'(a) = [f'(a)]^2 \geq 0$, $g'(a) = 1$. There are two cases
- $f'(a) = 1$.
- $f'(a) = -1$.
- Assume $f'(a) = 1$. In this case
- $g''(a) = f''(f(a))[f'(a)]^2 + f'(f(a)) f''(a) = 2f''(a) = 0$. Hence $f''(a) = 0$
- $g'''(a) = f'''(f(a)) f'(a) [f'(a)]^2 + 2f''(f(a)) f'(a) f''(a) + f''(f(a)) f'(a) f''(a) + f'(f(a))f'''(a) = 2f'''(a) < 0$. Hence $f'''(a) < 0$
- It follows that $a$ is an asymptotically stable equilibrium of (2)
- My question is how can we proceed when $f'(a) = -1$
- Theorem 1.16 states that if $f'(a) = -1$ and $-f'''(a) - 3/2(f''(a))^2 < 0$, then $a$ is asymptotically stable.
- But since this proposition is used to prove Theorem 1.16, using Theorem 1.16 to prove this proposition would be circular.
Hint: Whether or not a point is an asymptotically stable equilibrium point is a purely topological notion, and in this case using the definitions will suffice (note that if $f$ is continuous, then so is $g=f\circ f$). As a heuristic it might be useful to think of $g$ as a "time change" of $f$; under the action of $g$ everything that happens under the action of $f$ happens twice as fast (and vice versa: under the action of $f$ everything that happens under the action of $g$ happens twice as slow).