MHB What is the Riemannian distance between two points in the open unit disk?

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    2017
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The discussion focuses on finding the Riemannian distance between two points in the open unit disk, defined by the metric ds² = |dz|² / (1 - |z|²)². Participants are encouraged to derive a formula for this distance and apply it to the specific points -1/2 e^(iπ/4) and 1/2 e^(iπ/4). An extended timeframe for problem-solving is provided due to the holiday season. One participant, Serena, received recognition for correctly calculating the distance between the specified points. The thread emphasizes engagement with the problem and sharing solutions.
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Happy Holidays, everyone! Here is this week's POTW:

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Consider the open unit disk $\Bbb D\subset \Bbb C$ with Riemannian metric $ds^2 = \dfrac{\lvert dz\rvert^2}{(1 - \lvert z\rvert^2)^2}$. Find a formula for the (Riemannian) distance between two points in $\Bbb D$, and use it to find the distance between $-\frac{1}{2}e^{i\pi/4}$ and $\frac{1}{2}e^{i\pi/4}$.

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Due to the holiday break I’m giving an extra week to solve this problem. Happy New Year, everyone!
 
I like Serena gets honorable mention for his correct calculation for the Riemannian distance from $-\frac{1}{2}e^{i\pi/4}$ to $\frac{1}{2}e^{i\pi/4}$. You can read my solution below.
Given $z,w\in \Bbb D$, the Riemannian distance between $z$ and $w$ is given by

$$d(z,w) = \frac{1}{2}\log\frac{1 + \left\lvert\dfrac{z - w}{1 - \bar{z}w}\right\rvert}{1 - \left\lvert\dfrac{z - w}{1 - \bar{z}w}\right\rvert}$$ If $\gamma$ is a smooth curve in $\Bbb D$, set $\displaystyle\rho(\gamma) := \int_\gamma \frac{\lvert dz\rvert}{1 -\lvert z\rvert^2}$. For every isometry $\phi\in \operatorname{Isom}(\Bbb D)$, $\rho(\phi\circ \gamma) = \rho(\gamma)$. For by the Schwarz lemma, $\dfrac{\lvert \phi'(z)\rvert}{1 - \lvert z\rvert^2} \le \dfrac{1}{1 - \lvert z\rvert^2}$ for all $z\in \Bbb D$; hence

$$\rho(\phi\circ \gamma) = \int_\gamma \frac{\lvert \phi'(w)\rvert}{1 - \lvert \phi(w)\rvert^2}\lvert dw\rvert \le \int_\gamma \frac{\lvert dw\rvert}{1 - \lvert w\rvert^2} = \rho(\gamma)$$

and similarly $\rho(\gamma) = \rho(\phi^{-1}\circ \phi \circ \gamma) \le \rho(\phi\circ \gamma)$. Consequently, $d$ is invariant under the action of Möbius transformations on $\Bbb D$. Using the Möbius transformation $\phi : \Bbb D\to \Bbb D$ given by $\phi(c) := e^{i\theta}\dfrac{z - c}{1 - \bar{z}c}$ (where $\theta$ is chosen so that $\phi(w) \ge 0$), we have $d(z,w) = d(0, \phi(w))$. A geodesic joining two points on the real axis is a segment on the axis between the points, so $$d(z,w) = \int_0^{\phi(w)} \frac{dx}{1 - x^2} = \frac{1}{2}\log\frac{1 + \phi(w)}{1 - \phi(w)} = \frac{1}{2}\log \frac{1 + \left\lvert \dfrac{z - w}{1 - \bar{z}w}\right\rvert}{1 - \left\lvert \dfrac{z - w}{1 - \bar{z}w}\right\rvert}$$

Using this formula, we compute

$$d\left(-\frac{1}{2}e^{i\pi/4}, \frac{1}{2}e^{i\pi/4}\right) = \frac{1}{2}\log\frac{1 + \frac{4}{5}}{1 - \frac{4}{5}} = \frac{1}{2}\log 9 = \log 3$$