# Metaplectic group

In mathematics, the metaplectic group Mp$_{2n}$ is a double cover of the symplectic group Sp$_{2n}$. It can be defined over either real or p-adic numbers. The construction covers more generally the case of an arbitrary local or finite field, and even the ring of adeles.
The metaplectic group has a particularly significant infinite-dimensional linear representation, the Weil representation. It was used by André Weil to give a representation-theoretic interpretation of theta functions, and is important in the theory of modular forms of half-integral weight and the theta correspondence.

## Definition

The fundamental group of the symplectic Lie group Sp$_{2n}$(R) is infinite cyclic, so it has a unique connected double cover, which is denoted Mp$_{2n}$(R) and called the metaplectic group.
The metaplectic group Mp$_2$(R) is not a matrix group: it has no faithful finite-dimensional representations. Therefore, the question of its explicit realization is nontrivial. It has faithful irreducible infinite-dimensional representations, such as the Weil representation described below.
It can be proved that if F is any local field other than C, then the symplectic group Sp$_{2n}$(F) admits a unique perfect central extension with the kernel Z/2Z, the cyclic group of order 2, which is called the metaplectic group over F. It serves as an algebraic replacement of the topological notion of a 2-fold cover used when F = R. The approach through the notion of central extension is useful even in the case of real metaplectic group, because it allows a description of the group operation via a certain cocycle.

## Explicit construction for n = 1

In the case n = 1, the symplectic group coincides with the special linear group SL$_2$(R). This group biholomorphically acts on the complex upper half-plane by fractional-linear transformations, such as the Möbius transformation,
    $g\cdot z={\frac {az+b}{cz+d}}$
where
    $g={\begin{pmatrix}a&b\\c&d\end{pmatrix}}\in \operatorname {SL} _{2}(\mathbf {R} )$
is a real 2-by-2 matrix with the unit determinant and z is in the upper half-plane, and this action can be used to explicitly construct the metaplectic cover of SL$_2$(R).
The elements of the metaplectic group Mp$_2$(R) are the pairs (g, ε), where $g\in \operatorname {SL} _{2}(\mathbf {R} )$ and ε is a holomorphic function on the upper half-plane such that $\epsilon (z)^{2}=cz+d=j(g,z)$. The multiplication law is defined by:
    $(g_{1},\epsilon _{1})\cdot (g_{2},\epsilon _{2})=(g_{1}g_{2},\epsilon ),$ where $\epsilon (z)=\epsilon _{1}(g_{2}\cdot z)\epsilon _{2}(z).$
That this product is well-defined follows from the cocycle relation $j(g_{1}g_{2},z)=j(g_{1},g_{2}\cdot z)j(g_{2},z)$. The map
    $(g,\epsilon )\mapsto g$
is a surjection from Mp$_2$(R) to SL$_2$(R) which does not admit a continuous section. Hence, we have constructed a non-trivial 2-fold cover of the latter group.

## Construction of the Weil representation

The existence of the Weil representation can be proven abstractly, as follows. The Heisenberg group has an irreducible unitary representation on a Hilbert space ${\mathcal {H}}$, that is,
    $\rho :\mathbb {H} (V)\longrightarrow U({\mathcal {H}})$
with the center acting as multiplication by a given nonzero constant. The Stone–von Neumann theorem states that this representation is essentially unique: if $\rho '$ is another such representation, there exists an automorphism
    $\psi \in U({\mathcal {H}})$ such that $\rho '=\operatorname {Ad} _{\psi }(\rho )$.
and the conjugating automorphism is unique up to multiplication by a constant of modulus 1. So any automorphism of the Heisenberg group that induces the identity on the center acts on this representation ${\mathcal {H}}$—more precisely, the action is only well-defined up to multiplication by a nonzero constant.
The automorphisms of the Heisenberg group (fixing its center) form the symplectic group, so an action of these automorphisms is equivalent to an action of the symplectic group. But the action above is only defined up to multiplication by a nonzero constant, so an automorphism of the group is mapped to an equivalence class $[\psi ]\in \operatorname {PU} ({\mathcal {H}})$ of multiples of $\psi$. This is a projective representation, a homomorphism from the symplectic group to the projective unitary group of ${\mathcal {H}}$. The general theory of projective representations gives an action of some central extension of the symplectic group on ${\mathcal {H}}$. This central extension can be taken to be a double cover, which is the metaplectic group.
Concretely, in the case of Mp$_2$(R), the Hilbert space ${\mathcal {H}}$ is L$^2$(R), the square-integrable functions on the reals. The Heisenberg group is generated by translations and by multiplication by the functions e$^{ixy}$ of x, for y real. The action of the metaplectic group on ${\mathcal {H}}$—the Weil representation—is generated by the Fourier transform and multiplication by the functions exp(ix$^2$y) of x, for y real.

## Generalizations

Weil showed how to extend the theory above by replacing $\mathbb {R}$ by any locally compact abelian group G, which by Pontryagin duality is isomorphic to its dual (the group of characters). The Hilbert space H is then the space of all L$^2$ functions on G. The (analogue of) the Heisenberg group is generated by translations by elements of G, and multiplication by elements of the dual group (considered as functions from G to the unit circle). There is an analogue of the symplectic group acting on the Heisenberg group, and this action lifts to a projective representation on H. The corresponding central extension of the symplectic group is called the metaplectic group.
Some important examples of this construction are given by:
* G is a vector space over the reals of dimension n. This gives a metaplectic group that is a double cover of the symplectic group Sp$_{2n}$(R).
* More generally G can be a vector space over any local field F of dimension n. This gives a metaplectic group that is a double cover of the symplectic group Sp$_{2n}$(F).
* G is a vector space over the adeles of a number field (or global field). This case is used in the representation-theoretic approach to automorphic forms.
* G is a finite group. The corresponding metaplectic group is then also finite, and the central cover is trivial. This case is used in the theory of theta functions of lattices, where typically G will be the discriminant group of an even lattice.
* A modern point of view on the existence of the linear (not projective) Weil representation over a finite field, namely, that it admits a canonical Hilbert space realization, was proposed by David Kazhdan. Using the notion of canonical intertwining operators suggested by Joseph Bernstein, such a realization was constructed by Gurevich-Hadani.