# Atkin–Lehner theory

# Atkin–Lehner theory

In mathematics, **Atkin–Lehner theory** is part of the theory of modular forms, in which the concept of **newform** is defined in such a way that the theory of Hecke operators can be extended to higher level. A newform is a cusp form 'new' at a given *level* *N*, where the levels are the nested congruence subgroups:

of the modular group, with *N* ordered by divisibility. That is, if *M* divides *N*, Γ0(*N*) is a subgroup of Γ0(*M*). The **oldforms** for Γ0(*N*) are those modular forms *f(τ)* of level *N* of the form *g*(*d τ*) for modular forms *g* of level *M* with *M* a proper divisor of *N*, where *d* divides *N/M*. The newforms are defined as a vector subspace of the modular forms of level *N*, complementary to the space spanned by the oldforms, i.e. the orthogonal space with respect to the Petersson inner product.

The Hecke operators, which act on the space of all cusp forms, preserve the subspace of newforms and are self-adjoint and commuting operators (with respect to the Petersson inner product) when restricted to this subspace. Therefore, the algebra of operators on newforms they generate is a finite-dimensional C*-algebra that is commutative; and by the spectral theory of such operators, there exists a basis for the space of newforms consisting of eigenforms for the full Hecke algebra.

Atkin–Lehner involutions

Consider a Hall divisor *e* of *N*, which means that not only does *e* divide *N*, but also *e* and *N*/*e* are relatively prime (often denoted *e*||*N*). If *N* has *s* distinct prime divisors, there are 2*s* Hall divisors of *N*; for example, if *N* = 360 = 23⋅32⋅51, the 8 Hall divisors of *N* are 1, 23, 32, 51, 23⋅32, 23⋅51, 32⋅51, and 23⋅32⋅51.

For each Hall divisor *e* of *N*, choose an integral matrix *W**e* of the form

with det *W**e* = *e*. These matrices have the following properties:

The elements

*W**e**normalize*Γ0(*N*): that is, if*A*is in Γ0(*N*), then*W*−1**e**AW*e*is in Γ0(*N*).The matrix

*W*2*e*, which has determinant*e*2, can be written as*eA*where*A*is in Γ0(*N*). We will be interested in operators on cusp forms coming from the action of*W**e*on Γ0(*N*) by conjugation, under which both the scalar*e*and the matrix*A*act trivially. Therefore the equality*W*2*e*=*eA*implies that the action of*W**e*squares to the identity; for this reason, the resulting operator is called an**Atkin–Lehner involution**.If

*e*and*f*are both Hall divisors of*N*, then W*e*and W*f*commute modulo Γ0(*N*). Moreover, if we define*g*to be the Hall divisor*g*=*ef*/(*e*,*f*)2, their product is equal to W*g*modulo Γ0(*N*).If we had chosen a different matrix

*W*′*e*instead of*W**e*, it turns out that*W**e*≡*W*′*e*modulo Γ0(*N*), so*W**e*and*W*′*e*would determine the same Atkin–Lehner involution.

We can summarize these properties as follows. Consider the subgroup of GL(2,**Q**) generated by Γ0(*N*) together with the matrices *W**e*; let Γ0(*N*)+ denote its quotient by positive scalar matrices. Then Γ0(*N*) is a normal subgroup of Γ0(*N*)+ of index 2*s* (where *s* is the number of distinct prime factors of *N*); the quotient group is isomorphic to (**Z**/2**Z**)s and acts on the cusp forms via the Atkin–Lehner involutions.