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In the mathematical field of
representation theory Representation theory is a branch of mathematics that studies abstract algebraic structures by ''representing'' their elements as linear transformations of vector spaces, and studies modules over these abstract algebraic structures. In essen ...
, a reductive dual pair is a pair of subgroups (''G'', ''G''′) of the
isometry group In mathematics, the isometry group of a metric space is the set of all bijective isometries (i.e. bijective, distance-preserving maps) from the metric space onto itself, with the function composition as group operation. Its identity element is t ...
Sp(''W'') of a
symplectic vector space In mathematics, a symplectic vector space is a vector space ''V'' over a field ''F'' (for example the real numbers R) equipped with a symplectic bilinear form. A symplectic bilinear form is a mapping that is ; Bilinear: Linear in each argument ...
''W'', such that ''G'' is the
centralizer In mathematics, especially group theory, the centralizer (also called commutant) of a subset ''S'' in a group ''G'' is the set of elements \mathrm_G(S) of ''G'' such that each member g \in \mathrm_G(S) commutes with each element of ''S'', ...
of ''G''′ in Sp(''W'') and vice versa, and these groups act reductively on ''W''. Somewhat more loosely, one speaks of a dual pair whenever two groups are the mutual centralizers in a larger group, which is frequently a
general linear group In mathematics, the general linear group of degree ''n'' is the set of invertible matrices, together with the operation of ordinary matrix multiplication. This forms a group, because the product of two invertible matrices is again invertible ...
. The concept was introduced by Roger Howe in . Its strong ties with Classical Invariant Theory are discussed in .


Examples

* The full symplectic group ''G'' = Sp(''W'') and the two-element group ''G''′, the center of Sp(''W''), form a reductive dual pair. The double centralizer property is clear from the way these groups were defined: the centralizer of the group ''G'' in ''G'' is its center, and the centralizer of the center of any group is the group itself. The group ''G''′, consists of the identity transformation and its negative, and can be interpreted as the orthogonal group of a one-dimensional vector space. It emerges from the subsequent development of the theory that this pair is a first instance of a general family of dual pairs consisting of a symplectic group and an orthogonal group, which are known as ''type I irreducible reductive dual pairs''. * Let ''X'' be an ''n''-dimensional vector space, ''Y'' be its dual, and ''W'' be the
direct sum The direct sum is an operation between structures in abstract algebra, a branch of mathematics. It is defined differently, but analogously, for different kinds of structures. To see how the direct sum is used in abstract algebra, consider a mo ...
of ''X'' and ''Y''. Then ''W'' can be made into a symplectic vector space in a natural way, so that (''X'', ''Y'') is its lagrangian polarization. The group ''G'' is the general linear group GL(''X''), which acts tautologically on ''X'' and contragrediently on ''Y''. The centralizer of ''G'' in the symplectic group is the group ''G''′, consisting of linear operators on ''W'' that act on ''X'' by multiplication by a non-zero scalar λ and on ''Y'' by scalar multiplication by its inverse λ−1. Then the centralizer of ''G''′, is ''G'', these two groups act completely reducibly on ''W'', and hence form a reductive dual pair. The group ''G''′, can be interpreted as the general linear group of a one-dimensional vector space. This pair is a member of a family of dual pairs consisting of general linear groups known as ''type II irreducible reductive dual pairs''.


Structure theory and classification

The notion of a reductive dual pair makes sense over any field ''F'', which we assume to be fixed throughout. Thus ''W'' is a symplectic
vector space In mathematics and physics, a vector space (also called a linear space) is a set whose elements, often called '' vectors'', may be added together and multiplied ("scaled") by numbers called '' scalars''. Scalars are often real numbers, but ...
over ''F''. If ''W''1 and ''W''2 are two symplectic vector spaces and (''G''1, ''G''′1), (''G''2, ''G''′2) are two reductive dual pairs in the corresponding symplectic groups, then we may form a new symplectic vector space ''W'' = ''W''1 ⊕ ''W''2 and a pair of groups ''G'' = ''G''1 × ''G''2, ''G''′ = ''G''′1 × ''G''′,2 acting on ''W'' by isometries. It turns out that (''G'', ''G''′) is a reductive dual pair. A reductive dual pair is called reducible if it can be obtained in this fashion from smaller groups, and irreducible otherwise. A reducible pair can be decomposed into a direct product of irreducible ones, and for many purposes, it is enough to restrict one's attention to the irreducible case. Several classes of reductive dual pairs had appeared earlier in the work of
André Weil André Weil (; ; 6 May 1906 – 6 August 1998) was a French mathematician, known for his foundational work in number theory and algebraic geometry. He was a founding member and the ''de facto'' early leader of the mathematical Bourbaki group. ...
. Roger Howe proved a classification theorem, which states that in the irreducible case, those pairs exhaust all possibilities. An irreducible reductive dual pair (''G'', ''G''′) in Sp(''W'') is said to be of type II if there is a lagrangian subspace ''X'' in ''W'' that is invariant under both ''G'' and ''G''′, and of type I otherwise. An archetypical irreducible reductive dual pair of type II consists of a pair of
general linear group In mathematics, the general linear group of degree ''n'' is the set of invertible matrices, together with the operation of ordinary matrix multiplication. This forms a group, because the product of two invertible matrices is again invertible ...
s and arises as follows. Let ''U'' and ''V'' be two vector spaces over ''F'', ''X'' = ''U'' ⊗''F'' ''V'' be their tensor product, and ''Y'' = Hom''F''(''X'', ''F'') its dual. Then the direct sum ''W'' = ''X'' ⊕ ''Y'' can be endowed with a symplectic form such that ''X'' and ''Y'' are lagrangian subspaces, and the restriction of the symplectic form to ''X'' × ''Y'' ⊂ ''W'' × ''W'' coincides with the pairing between the vector space ''X'' and its dual ''Y''. If ''G'' = GL(''U'') and ''G''′ = GL(''V''), then both these groups act linearly on ''X'' and ''Y'', the actions preserve the symplectic form on ''W'', and (''G'', ''G''′) is an irreducible reductive dual pair. Note that ''X'' is an invariant lagrangian subspace, hence this dual pair is of type II. An archetypical irreducible reductive dual pair of type I consists of an
orthogonal group In mathematics, the orthogonal group in dimension , denoted , is the group of distance-preserving transformations of a Euclidean space of dimension that preserve a fixed point, where the group operation is given by composing transformations. ...
and a symplectic group and is constructed analogously. Let ''U'' be an orthogonal vector space and ''V'' be a symplectic vector space over ''F'', and ''W'' = ''U'' ⊗''F'' ''V'' be their tensor product. The key observation is that ''W'' is a symplectic vector space whose bilinear form is obtained from the product of the forms on the tensor factors. Moreover, if ''G'' = O(''U'') and ''G''′ = Sp(''V'') are the
isometry group In mathematics, the isometry group of a metric space is the set of all bijective isometries (i.e. bijective, distance-preserving maps) from the metric space onto itself, with the function composition as group operation. Its identity element is t ...
s of ''U'' and ''V'', then they act on ''W'' in a natural way, these actions are symplectic, and (''G'', ''G''′) is an irreducible reductive dual pair of type I. These two constructions produce all irreducible reductive dual pairs over an algebraically closed field ''F'', such as the field C of
complex number In mathematics, a complex number is an element of a number system that extends the real numbers with a specific element denoted , called the imaginary unit and satisfying the equation i^= -1; every complex number can be expressed in the for ...
s. In general, one can replace vector spaces over ''F'' by vector spaces over a
division algebra In the field of mathematics called abstract algebra, a division algebra is, roughly speaking, an algebra over a field in which division, except by zero, is always possible. Definitions Formally, we start with a non-zero algebra ''D'' over a f ...
''D'' over ''F'', and proceed similarly to above to construct an irreducible reductive dual pair of type II. For type I, one starts with a division algebra ''D'' with involution τ, a
hermitian form In mathematics, a sesquilinear form is a generalization of a bilinear form that, in turn, is a generalization of the concept of the dot product of Euclidean space. A bilinear form is linear in each of its arguments, but a sesquilinear form allows ...
on ''U'', and a skew-hermitian form on ''V'' (both of them non-degenerate), and forms their tensor product over ''D'', ''W'' = ''U'' ⊗''D'' ''V''. Then ''W'' is naturally endowed with a structure of a symplectic vector space over ''F'', the isometry groups of ''U'' and ''V'' act symplectically on ''W'' and form an irreducible reductive dual pair of type I. Roger Howe proved that, up to an isomorphism, any irreducible dual pair arises in this fashion. An explicit list for the case ''F'' = R appears in .


See also

* Howe correspondence between representations of elements of a reductive dual pair. *
Heisenberg group In mathematics, the Heisenberg group H, named after Werner Heisenberg, is the group of 3×3 upper triangular matrices of the form ::\begin 1 & a & c\\ 0 & 1 & b\\ 0 & 0 & 1\\ \end under the operation of matrix multiplication. Element ...
* Metaplectic group


References

* * . * . * {{citation, last2=Wallach, first2=Nolan R., last1=Goodman, first1=Roe, year=1998, title=Representations and Invariants of the Classical Groups, publisher= Cambridge University Press, isbn= 0-521-66348-2. Representation theory