In the usual theory of classical modular forms, the modular forms defined to be "holomorphic at the cusp infinity". I do not know what this should mean? can anyone explain it for me?
Thanks
In the usual theory of classical modular forms, the modular forms defined to be "holomorphic at the cusp infinity". I do not know what this should mean? can anyone explain it for me?
Thanks
For simplicity, let's just consider modular forms (of weight $k$) of the modular group $SL(2,\mathbb{Z})$, i.e. holomorphic functions $f \colon \mathbb{H} \to \mathbb{C}$ satisfying two other conditions, the second being the "holomorphicity at $\infty$" in which we're interested.
The first condition is that $f$ has a nice symmetry under the action of $SL(2,\mathbb{Z})$; that is, $$f \left( \begin{pmatrix} a & b \\ c & d \end{pmatrix} \cdot z \right) = (cz+d)^k f(z)$$ and this must hold for all matrices $\begin{pmatrix} a & b \\ c & d \end{pmatrix} \in SL(2,\mathbb{Z})$. If we take the matrix $\begin{pmatrix} 1 & 1 \\ 0 & 1 \end{pmatrix}$ in the above equation, then we get that $f(z) = f(z+1)$ i.e. our modular form $f$ is periodic, hence has a Fourier series expansion. Write $$ f(z) = \sum_{n=0}^{\infty} a_n e^{2\pi inz}. $$ A common convention is to make the change of variable $q := e^{2\pi inz}$ and to view $f$ as a holomorphic function in $q$. The function $z \mapsto e^{2\pi inz}$ is a conformal map sending the upper half plane $\mathbb{H}$ to the punctured unit disc, where the point $i\infty$ is sent to the origin. Therefore, the modular form $f$ can be viewed as the holomorphic function $q \mapsto \sum_{n=0}^{\infty} a_n q^n$, from the punctured unit disc.
How does this help us understand "holomorphicity at $\infty$"? The second condition in the definition of a modular form, namely this "holomorphic at $\infty$" condition, says that $f(q)$ can be extended to a holomorphic function on the whole unit disc, i.e. it can be analytically continued through the puncture at the origin. By Riemann's theorem on removable singularities, this occurs when $f(q)$ is bounded is a neighbourhood of the origin; so you will often see the "holomorphic at $\infty$" condition written as "bounded at $\infty$" instead.
Two comments on this approach: one doesn't need to translate everything to the unit disc (as I did above) if we view $f$ as a function from a subset of the Riemann sphere. Second, another way to characterize this "holomorphic at $\infty$" condition is to say that $f$ defines a holomorphic function on the Riemann surface $SL(2,\mathbb{Z}) \backslash \mathbb{H}$ (this is the classical modular curve, which has a cusp at $i\infty$).
An excellent, but advanced, reference for this material are the first few chapters of Milne's course notes on modular forms. They are freely available here.