Isometry $f:M\to M$ has a fixed point $p$ with $df_p=\text{id} \Rightarrow f=\text{id}$

differential-geometryisometryriemannian-geometry

I'm trying to prove whether or not the following statement is true:

If $(M,g)$ is a connected Riemannian manifold and $f:M\to M$ is an isometry, then $f=\text{id}_M\Leftrightarrow $ there is some $p\in M$ with $f(p)=p$ and $df_p=\text{id}$.

$(\Rightarrow)$ is obvious.

For $(\Leftarrow)$, I know how to prove it when $(M,g)$ is complete: for any $q\in M$ there is a geodesic $\gamma$ joining $p,q$. Since $f$ is an isometry, $f\circ\gamma$ is a geodesic starting at $f\circ\gamma(0)=f(p)=p$ with velocity $(f\circ\gamma)'(0)=df_p(\gamma'(0))=\gamma'(0)$ so $f\circ\gamma=\gamma$ by uniqueness of geodesics. In particular, $f(q)=q$, which means $f=\text{id}_M$ since $q$ is arbitrary.

For the general case, I don't know how to prove it or find a counterexample.

Best Answer

If the manifold is connected, the goal is to show that the agreement set $$A = \{p \in M \mid f(p) = p \quad\mbox{and}\quad {\rm d}f_p = {\rm Id}_{T_pM}\}$$is non-empty, open, and closed. It is non-empty by assumption. Closed by smoothness of $f$ (which implies continuity of $f$ and of its differential). It remains to show that $A$ is open. So let $p \in A$, and let $D_p\subseteq T_pM$ be an open and starshaped domain for which $\exp_p\colon D_p \to \exp_p[D_p]\subseteq M$ is a diffeomorphism. Then $p \in \exp_p[D_p]$ is open, and we can show that $\exp_p[D_p] \subseteq A$.

If $q \in \exp_p[D_p]$, there is $v \in D_p$ such that the geodesic segment $\gamma\colon [0,1] \to M$ given by $\gamma(t) = \exp_p(tv)$ always lies inside $\exp_p[D_p]$, with $\gamma(1) =q$. By the uniqueness argument you mentioned yourself, we have that $f\circ \gamma = \gamma$. This in particular shows that $f(q) = q$. But since $f$ is an isometry, we have that

$$ f\circ \exp_p = \exp_{f(p)} \circ \,{\rm d}f_p\implies f \circ \exp_p = \exp_q.$$Differentiating at $0$ and using that ${\rm d}(\exp_p)_0 = {\rm Id}_{T_pM}$ and ${\rm d}(\exp_q)_0 = {\rm Id}_{T_qM}$ gives that ${\rm d}f_q={\rm Id}_{T_qM}$ as well.


The real consequence here is that if you have two isometries $f,\widetilde{f}\colon M \to M'$ between (connected) pseudo-Riemannian manifolds (positiveness of the metric was irrelevant here), then if there is $p \in M$ with $f(p) = \widetilde{f}(p)$ and ${\rm d}f_p = {\rm d}\widetilde{f}_p$, we conclude that $f=\widetilde{f}$.

The result remains true if we replace "isometries" by "pseudo-Riemannian submersions", provided that the fundamental tensors associated to both submersions are also equal (that's the price one pays for freeing themselves of the dimension constraint). See the paper The Fundamental Equations of a Submersion, by Barrett O'Neill.

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