In mathematics, a cusp neighborhood is defined as a set of points near a cusp singularity.[1]
The cusp neighborhood for a hyperbolic Riemann surface can be defined in terms of its Fuchsian model.[2] Suppose that the Fuchsian group G contains a parabolic element g. For example, the element t ∈ SL(2,Z) where
t(z)=\begin{pmatrix}1&1\ 0&1\end{pmatrix}:z=
1 ⋅ z+1 | |
0 ⋅ z+1 |
=z+1
is a parabolic element. Note that all parabolic elements of SL(2,C) are conjugate to this element. That is, if g ∈ SL(2,Z) is parabolic, then
g=h-1th
The set
U=\{z\inH:\Imz>1\}
where H is the upper half-plane has
\gamma(U)\capU=\emptyset
for any
\gamma\inG-\langleg\rangle
\langleg\rangle
E=U/\langleg\rangle
Here, E is called the neighborhood of the cusp corresponding to g.
\left\{z\inH:\left|z\right|>1,\left|Re(z)\right|<
1 | |
2 |
\right\}
of the modular group, as would be appropriate for the choice of T as the parabolic element. When integrated over the volume element
d\mu= | dxdy |
y2 |
the result is trivially 1. Areas of all cusp neighborhoods are equal to this, by the invariance of the area under conjugation.