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		<title>Cusp form</title>
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		<summary type="html">&lt;p&gt;129.64.0.36: &lt;/p&gt;
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&lt;div&gt;In [[number theory]], a branch of [[mathematics]], a &#039;&#039;&#039;cusp form&#039;&#039;&#039; is a particular kind of [[modular form]] with a zero constant coefficient in the [[Fourier series]] [[Series expansion|expansion]].&lt;br /&gt;
&lt;br /&gt;
==Introduction==&lt;br /&gt;
A cusp form is distinguished in the case of modular forms for the [[modular group]] by the vanishing of the constant coefficient &#039;&#039;a&#039;&#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; in the [[Fourier series]] expansion (see [[q-expansion|&#039;&#039;q&#039;&#039;-expansion]])&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum a_n q^n.&amp;lt;/math&amp;gt;&lt;br /&gt;
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This Fourier expansion exists as a consequence of the presence in the modular group&#039;s action on the [[upper half-plane]] via the transformation&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;z\mapsto z+1.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For other groups, there may be some translation through several units, in which case the Fourier expansion is in terms of a different parameter.  In all cases, though, the limit as &#039;&#039;q&#039;&#039; → 0 is the limit in the upper half-plane as the [[imaginary part]] of &#039;&#039;z&#039;&#039; → ∞. Taking the quotient by the modular group, this limit corresponds to a [[Cusp (singularity)|cusp]] of a [[modular curve]] (in the sense of a point added for [[compactification (mathematics)|compactification]]). So, the definition amounts to saying that a cusp form is a modular form that vanishes at a cusp. In the case of other groups, there may be several cusps, and the definition becomes a modular form vanishing at &#039;&#039;all&#039;&#039; cusps. This may involve several expansions.&lt;br /&gt;
&lt;br /&gt;
==Dimension==&lt;br /&gt;
The dimensions of spaces of cusp forms are, in principle, computable via the [[Riemann–Roch theorem]].  For example, the [[Ramanujan tau function]] &#039;&#039;τ&#039;&#039;(&#039;&#039;n&#039;&#039;) arises as the sequence of Fourier coefficients of the cusp form of weight 12 for the modular group, with &#039;&#039;a&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;amp;nbsp;=&amp;amp;nbsp;1. The space of such forms has dimension&amp;amp;nbsp;1, which means this definition is possible; and that accounts for the action of [[Hecke operator]]s on the space being by [[scalar multiplication]] (Mordell&#039;s proof of Ramanujan&#039;s identities). Explicitly it is the &#039;&#039;&#039;modular discriminant&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Delta(z,q),&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
which represents (up to a [[normalizing constant]]) the [[discriminant]] of the cubic on the right side of the [[Weierstrass equation]] of an [[elliptic curve]]; and the 24-th power of the [[Dedekind eta function]]. The Fourier coefficients here are written&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\tau(n)&amp;lt;/math&amp;gt;&lt;br /&gt;
and called &#039;[[Ramanujan tau function|Ramanujan&#039;s tau function]]&#039;, with the normalization &#039;&#039;τ&#039;&#039;(1) = 1.&lt;br /&gt;
&lt;br /&gt;
==Related concepts==&lt;br /&gt;
In the larger picture of [[automorphic form]]s, the cusp forms are complementary to [[Eisenstein series]], in a &#039;&#039;discrete spectrum&#039;&#039;/&#039;&#039;continuous spectrum&#039;&#039;, or &#039;&#039;discrete series representation&#039;&#039;/&#039;&#039;induced representation&#039;&#039; distinction typical in different parts of [[spectral theory]]. That is, Eisenstein series can be &#039;designed&#039; to take on given values at cusps. There is a large general theory, depending though on the quite intricate theory of parabolic subgroups, and corresponding [[cuspidal representation]]s.&lt;br /&gt;
&lt;br /&gt;
Consider &amp;lt;math&amp;gt;P=MU&amp;lt;/math&amp;gt; a standard parabolic subgroup of some reductive group &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; (over &amp;lt;math&amp;gt;\mathbb{A}&amp;lt;/math&amp;gt;, the [[adele ring]]), an automorphic form &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; on &amp;lt;math&amp;gt;U(\mathbb{A})M(k)\backslash G&amp;lt;/math&amp;gt; is called cuspidal if for all parabolic subgroups &amp;lt;math&amp;gt;P&#039;&amp;lt;/math&amp;gt; such that &amp;lt;math&amp;gt;P_0\subset P&#039;\subsetneq P&amp;lt;/math&amp;gt; we have &amp;lt;math&amp;gt;\phi_{P&#039;}=0&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;P_0&amp;lt;/math&amp;gt; is the standard minimal parabolic subgroup. The notation &amp;lt;math&amp;gt;\phi_{P}&amp;lt;/math&amp;gt; for &amp;lt;math&amp;gt;P=MU&amp;lt;/math&amp;gt; is defined as &amp;lt;math&amp;gt;\phi_P (g) =\int_{U(k)\backslash U(\mathbb{A})} \phi(ug) du&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*[[Jean-Pierre Serre|Serre, Jean-Pierre]], &#039;&#039;A Course in Arithmetic&#039;&#039;, [[Graduate Texts in Mathematics]], No. 7, [[Springer Science+Business Media|Springer-Verlag]], 1978. {{ISBN|0-387-90040-3}}&lt;br /&gt;
*[[Goro Shimura|Shimura, Goro]], &#039;&#039;An Introduction to the Arithmetic Theory of Automorphic Functions&#039;&#039;, [[Princeton University Press]], 1994. {{ISBN|0-691-08092-5}}&lt;br /&gt;
*[[Stephen Gelbart|Gelbart, Stephen]], &#039;&#039;Automorphic Forms on Adele Groups&#039;&#039;, Annals of Mathematics Studies, No. 83, Princeton University Press, 1975. {{ISBN|0-691-08156-5}}&lt;br /&gt;
* [[Colette Moeglin|Moeglin C]], [[Jean-Loup Waldspurger|Waldspurger JL]] &#039;&#039;Spectral Decomposition and Eisenstein Series: A Paraphrase of the Scriptures&#039;&#039;, Schneps L, trans. [[Cambridge University Press]]; 1995. {{ISBN|978-0521418935}}&lt;br /&gt;
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[[Category:Modular forms]]&lt;/div&gt;</summary>
		<author><name>129.64.0.36</name></author>
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