Symplectic group

The Lie group of linear transformations preserving a nondegenerate alternating form on .
Symplectic group

Definition

Let JJ be the standard symplectic matrix

J=(0InIn0), J=\begin{pmatrix}0&I_n\\-I_n&0\end{pmatrix},

so the bilinear form ω(u,v)=uTJv\omega(u,v)=u^T J v on R2n\mathbb R^{2n} is nondegenerate and skew-symmetric. The real symplectic group is

Sp(2n,R)={AGL(2n,R)ATJA=J}. \mathrm{Sp}(2n,\mathbb R)=\{A\in GL(2n,\mathbb R)\mid A^T J A = J\}.

This is a closed subgroup of the , hence a Lie subgroup by the .

More generally, for any field F\mathbb F of characteristic 2\neq 2, one defines Sp(2n,F)\mathrm{Sp}(2n,\mathbb F) as the group preserving a fixed nondegenerate alternating form; different choices are conjugate in GL(2n,F)GL(2n,\mathbb F).

Lie algebra

The Lie algebra of Sp(2n,R)\mathrm{Sp}(2n,\mathbb R) is the , obtained by differentiating the defining equation ATJA=JA^TJA=J at the identity.

Context

Sp(2n,R)\mathrm{Sp}(2n,\mathbb R) is the basic symmetry group of linear symplectic geometry and Hamiltonian mechanics: it preserves the standard symplectic form and hence the canonical Poisson structure on R2n\mathbb R^{2n}. In representation theory, its complexification corresponds to the simple Lie algebra of type CnC_n (compare and ).