About the Poincaré metric isometry and automorphism on the unit disc

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Consider two domains $\Omega_1$ and $\Omega_2$ in $\mathbb{C}$ with the corresponding metrics $g|d z|^2$ and $h|d w|^2$ respectively. Let $d_1$ be the distance function induced from $g|d z|^2$, and $d_2$ that from $h|d w|^2$. We say a map $f$ smooth if it is $C^{\infty}$ as a map from $\Omega_1 \subset \mathbb{R}^2$ to $\Omega_2 \subset \mathbb{R}^2$. Given a smooth bijection $f: \Omega_1 \rightarrow \Omega_2$, we call $f$ is an isometry if $f$ is distance-preserving in the sense that $d_1(z, w)=d_2(f(z), f(w))$ for any two points $z, w \in \Omega_1$.

Consider the unit disk $\mathbb{D}$ with its standard Poincaré metric. $$ d s_P^2=\frac{4}{\left(1-|z|^2\right)^2}|d z|^2 . $$

In the lecture we checked that any automorphism (holomorphic bijection) of $\mathbb{D}$ must be a holomorphic isometry. As a corollary we solved the corresponding distance function $d$ (called the Poincaré distance) induced from the Poincaré metric.

Question:

Given any isometry $f$ of $\mathbb{D}$ with respect to the Poincare distance, then either $f$ is an automorphism of $\mathbb{D}$ or its conjugate $\bar{f}$ is so}(why?). If we drop the assumption that an isometry is smooth, can we get the same conclusion?

I can only figure out $|f(z)|$ which is equal to $|\frac{z-\beta}{1-\bar{\beta}z}|$(where $\beta=f^{-1}(0)$).S ince $d(0,z)=\ln^{\frac{1-|z|}{1+|z|}}$ ,f is an isometry , thus $d(\beta,z)=d(0,f(z))$, and any automorphism of D is a holomorphic isometry. We have $d(\beta,z)=d(0,\frac{z-\beta}{1-\bar{\beta}z})=d(0,f(z))$, so this is all I can get. But how to proof either $f$ or $\bar{f}$ is actually equal to $\frac{z-\beta}{1-\bar{\beta}z}e^{i\theta}$?

This is my first time to ask questions in this community. Is there anyone who can help me?

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By comments from @ziqishen, its enough to consider $f(0) = 0$. So lets assume $f(0) = 0$. Since we have, $d(0,z) = d(f(0), f(z))$, we get, $|z| = \frac{|f(z)-f(0)|}{|1-f(0)^* f(z)|} \implies z = \frac{(f(z)-f(0))e^{j A(z)}}{1-f(0)^* f(z)} $.

Hence if $f(0) = 0$, we have that, $|f(z)| = |z|$. Hence $f(z) = ze^{j A(z)}$.

Let $A(z) \in [-\pi,\pi)$.

Prove that $\frac{|r_1 - r_2 e^{j \theta}|}{|1-r_1 r_2 e^{j \theta}|} = constant < 1$ has a unique solution $\gamma$ with $\theta = + \gamma$ or $\theta = - \gamma$ for fixed $r_1,r_2 \neq 0$.

$ d(f(r_1),f(r_2)) = d(r_1,r_2) = d(r_1 e^{j \theta},r_2 e^{j \theta}) = d(f(r_1 e^{j \theta}),f(r_2 e^{j \theta}))$

Note that $f(z) = z e^{j A(z)}$. Using this in above equation we get: $d(r_1,r_2) = d(f(r_1),f(r_2)) = d(f(r_1 e^{j \theta}),f(r_2 e^{j \theta})) \implies \frac{|r_1 - r_2|}{|1-r_1 r_2|} = \frac{|r_1 - r_2 e^{j (A(r_1)-A(r_2)}|}{|1-r_1 r_2 e^{j (A(r_1)-A(r_2)}|} = \frac{|r_1 - r_2 e^{j (A(r_1 e^{j \theta})-A(r_2 e^{j \theta})}|}{|1+r_1 r_2 e^{j (A(r_1 e^{j \theta})-A(r_2 e^{j \theta})}|} $.

Hence $e^{j (A(r_1 e^{j \theta})-A(r_2 e^{j \theta}) )}= e^{j(A(r_1)-A(r_2) )}= 1$ for fixed $r_1$ and $r_2$.

Hence for a fixed $r^*$ and for every other $r, \theta$, $e^{j(A(r e^{j \theta}))}= e^{j A(r^* e^{j \theta})}$.

Now by similar argument i.e., with $r_1 = r_2 = r$, $e^{j(A(r e^{j (h+\theta)}) - A(r e^{j \theta}))} = e^{j \pm (A(r e^{j h}) - A(r))} = e^{j \pm h}$

Using above, now assuming continuity of derivative of $g(t) = A(re^{jt})$, except at points where $A(re^{j \theta}) = -\pi$ (these points are assumed to be finitely many), the derivative of $A(re^{j\theta})$ w.r.t $\theta$ exists with derivative $\pm 1$, and we have $A(re^{j \theta})$ is linear in $\theta$ for a fixed $r$ i.e., of the form $s(r) \theta + g(r)$ with $s(r) = \pm 1$.

But by $A(r e^{j \theta}) = A(r^* e^{j \theta})$, we have that $s(r) = s(r^*) =\pm 1$ and $g(r) = g(r^*)$.

we have that $f(r e^{j \theta}) = r e^{j(s \theta + g)}$ for some constants $s=\pm 1, g$.