Let $f: \mathbb{R} \to \mathbb{R}$ be a $C^{\infty}$ differentiable function such that $$0=f(0)=f'(0)=...=f^{(n-1)} (0), $$ and $f^{(n)} (0) \neq 0$.
Show that there exists a diffeomorphism around $0$, say $h: ( \mathbb{R} , 0 ) \to ( \mathbb{R} , 0 ) $ such that
$f\circ h (x) = x^n $ if $n$ is odd, and
$f\circ h (x) = -x^n $ if $f^{(n)} (0) < 0$ and $n$ is even.
I think I should use the Taylor series of $f$ around $0$, but then I don't have any clue about how to proceed. Any help would be very appreciated. Thanks!
We can follow Morse lemma's proof closely and see that it works out fine. As in that case, we can take advantage of the following lemma:
This last observation is trivial from the equation, but is worthy pointing out. For a proof, just notice that $g(x)=\int_0^1(g(tx))'dt=\int_0^1g'(tx)xdt=x\int_0^1g'(tx)dt,$ so that $k(x)=\int_0^1g'(tx)dt$ gives the function we want.
Suppose now, for the sake of exposition, that $n$ is big enough. We then have $f(x)=xf_1(x)$ for some $f_1(x)$. Since $f_1(0)=f'(0)=0$, we can apply the result again to $f_1$, yielding that $f_1(x)=xf_2(x)$ for some $f_2(x)$, and therefore $f(x)=x^2f_2(x)$.
Note that there is a little problem now: a priori we don't know that $f_2(0)=0$, since $f_2(0)=f_1'(0)$, not $f'(0)$. Luckily we have that the proof of the lemma tells us that $f_2(x)=\int_0^1f_1'(tx)dt=\int_0^1\int_0^1f''(stx)sdsdt.$ Therefore, $f_2(0)=0$. (Actually, you can just use Taylor's theorem on $f$ and take the limit on $\frac{f(x)}{x^2}$ to conclude that $f_2(0)=0$.) Likewise, $f(x)=x^3f_3(x)$... until $f(x)=x^nf_n(x),$ where $f_n(0)=\frac{1}{n!}f^{(n)}(0)$.
Since $f_n(0) \neq 0$, either $\sqrt[n]{f_n(x)}$ is smooth on a neighbourhood of zero or $\sqrt[n]{-f_n(x)}$ is, depending on whether $f_n(0)$ is positive or negative and if it is the case that $n$ is even of course. In any case, let $g(x)$ be the correct one. Then, $f(x)=(xg(x))^n$ or $f(x)=-(xg(x))^n$ if $n$ is even and $f^{(n)}(0) <0$. By letting $u(x)=xg(x)$, we have that $u'(x)=g(x)+xg'(x)$, and thus $u'(0)=g(0) \neq 0$. By the inverse function theorem, $u$ is a diffeomorphism near $0$ and we've found our $h$: indeed, $f (x)=\pm(u(x))^n,$ thus $f(u^{-1}(x))=\pm x^n.$ (Where I've already made the observation about when it is $+$ or $-$.) Letting $h:=u^{-1}$ then suffices.