A horosphere in is an isometric image of a horizontal plane r=r0>0r=r_0>0 in the upper-half-space model

H3={(z,r):zC, r>0},ds2=(dz2+dr2)/r2.\mathbb H^3=\{(z,r):z\in\mathbb C,\ r>0\},\qquad ds^2=(|dz|^2+dr^2)/r^2.

The point \infty is the ideal center of a horizontal horosphere; isometries transport it to the center of the image horosphere.

Other centers

Horospheres centered at a finite boundary point are Euclidean spheres tangent to r=0r=0, with the tangency point omitted. The induced metric on a horizontal horosphere is dz2/r02|dz|^2/r_0^2, so it is intrinsically Euclidean.