Simple Closed Hyperbolic Geodesics on Punctured Spheres Thinking of $\mathbb {CP^1}$ as the sphere $S^2\subset\mathbb R^3$, we can define the notion of a circle on it to be a subset that is got by a hyperplane section of $S^2$ inside $\mathbb R^3$. This notion is known to be invariant under the complex automorphism group $PSL_2(\mathbb C)$ of $\mathbb {CP^1}$.
Suppose $n\ge 3$ is an integer. Then, it is known that the complement of $n$ distinct points $\{z_1,\ldots,z_n\}$ on $\mathbb {CP^1}$ carries a unique complete hyperbolic conformal metric of finite area, call it $g$. It is also known that if $\gamma$ is a simple closed curve on $X = \mathbb {CP^1}-\{z_1,\ldots,z_n\}$ which is homotopically non-trivial, then it is homotopic to a unique simple closed geodesic for $g$. Let us continue to denote this by $\gamma$. Is it then true that $\gamma\subset \mathbb {CP^1}$ is a circle in the sense of the previous paragraph?
 A: Unless I misunderstand the question, the answer is no. The homotopy class of the circle is determined by the partition it determines on the set of marked points, so there are only finitely many homotopy classes. By contrast, there are infinitely many homotopy classes of simple closed geodesics as long as the number of marked points is greater than $3.$
See, e.g.
Rivin, Igor, Simple curves on surfaces, Geom. Dedicata 87, No. 1-3, 345-360 (2001). ZBL1002.53027.
A: If the points are (setwise) invariant under reflection through a plane perpendicular to the sphere, then the the great circle of the reflection plane intersecting the sphere will be geodesic in the hyperbolic metric on the complement of the points. More generally one may consider inversions through spheres preserving the points (conformally equivalent to the plane example). It seems unlikely otherwise that a hyperbolic geodesic could be a circle (for example, one cannot just rotate the two hemispheres in the symmetric situation above, since the great circle will likely not be isometric to the hyperbolic geodesic). If we had a single configuration with two disjoint hyperbolic geodesic circles, we could get infinitely many more by cutting along the two circles, and doing inversions of the annulus through them $n$ times, then capping off with the disks on either end. But I suspect such examples are unlikely to exist.  
Here are pictures of hyperbolic geodesic curves in the 4-punctured sphere iterated by a braid (one puncture is at $\infty$). The first blue curve is a circle (stereographic projection will take it to a circle on the sphere). The colored circles surround the punctures, and are horocycles, not round circles.  
 





