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Symplectic vector space
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==Subspaces== Let ''W'' be a [[linear subspace]] of ''V''. Define the '''symplectic complement''' of ''W'' to be the subspace :<math>W^\perp = \{v \in V \mid \omega(v,w) = 0 \mbox{ for all } w \in W\}.</math> The symplectic complement satisfies: :<math>\begin{align} \left(W^\perp\right)^\perp &= W \\ \dim W + \dim W^\perp &= \dim V. \end{align}</math> However, unlike [[orthogonal complement]]s, ''W''<sup>β₯</sup> β© ''W'' need not be 0. We distinguish four cases: * ''W'' is '''symplectic''' if {{nowrap|1=''W''<sup>β₯</sup> β© ''W'' = {0}}}. This is true [[if and only if]] ''Ο'' restricts to a nondegenerate form on ''W''. A symplectic subspace with the restricted form is a symplectic vector space in its own right. * ''W'' is '''isotropic''' if {{nowrap|''W'' β ''W''<sup>β₯</sup>}}. This is true if and only if ''Ο'' restricts to 0 on ''W''. Any one-dimensional subspace is isotropic. * ''W'' is '''coisotropic''' if {{nowrap|''W''<sup>β₯</sup> β ''W''}}. ''W'' is coisotropic if and only if ''Ο'' descends to a nondegenerate form on the [[Quotient space (linear algebra)|quotient space]] ''W''/''W''<sup>β₯</sup>. Equivalently ''W'' is coisotropic if and only if ''W''<sup>β₯</sup> is isotropic. Any [[codimension]]-one subspace is coisotropic. * ''W'' is '''Lagrangian''' if {{nowrap|1=''W'' = ''W''<sup>β₯</sup>}}. A subspace is Lagrangian if and only if it is both isotropic and coisotropic. In a finite-dimensional vector space, a Lagrangian subspace is an isotropic one whose dimension is half that of ''V''. Every isotropic subspace can be extended to a Lagrangian one. Referring to the canonical vector space '''R'''<sup>2''n''</sup> above, * the subspace spanned by {''x''<sub>1</sub>, ''y''<sub>1</sub>} is symplectic * the subspace spanned by {''x''<sub>1</sub>, ''x''<sub>2</sub>} is isotropic * the subspace spanned by {''x''<sub>1</sub>, ''x''<sub>2</sub>, ..., ''x''<sub>''n''</sub>, ''y''<sub>1</sub>} is coisotropic * the subspace spanned by {''x''<sub>1</sub>, ''x''<sub>2</sub>, ..., ''x''<sub>''n''</sub>} is Lagrangian.
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