Definition

Let (V,ω)(V,\omega) be a finite-dimensional , and let WVW\subseteq V be a . The subspace WW is isotropic if

ωW×W=0.\omega|_{W\times W}=0.

Equivalently, every vector in WW is symplectically orthogonal to every other vector in WW, or

WWω,W\subseteq W^\omega,

where WωW^\omega is the . Isotropy is a condition on the whole subspace, not merely the automatic identities ω(w,w)=0\omega(w,w)=0 for individual vectors.

Dimension bound

If dimV=2n\dim V=2n, then

dimW+dimWω=2n.\dim W+\dim W^\omega=2n.

The inclusion WWωW\subseteq W^\omega therefore implies dimWn\dim W\leq n. An isotropic subspace of the maximal possible dimension nn satisfies W=WωW=W^\omega and is called Lagrangian.

Examples and contrasts

Every one-dimensional subspace is isotropic because an alternating form vanishes on pairs of proportional vectors. In a , span(e1,,ek)\operatorname{span}(e_1,\ldots,e_k) is isotropic for knk\leq n. By contrast, span(e1,f1)\operatorname{span}(e_1,f_1) is a , not an isotropic one.

Quotients and geometry

The restriction of ω\omega to WωW^\omega has kernel WW when WW is isotropic. Hence it descends to a nondegenerate alternating form on Wω/WW^\omega/W. Pointwise isotropic similarly define ; the present knowl concerns the underlying linear notion.

References
  1. Dusa McDuff and Dietmar Salamon, Introduction to Symplectic Topology, 3rd ed., Oxford University Press, 2017. DOI record. Relevant: Chapter 2, isotropic, coisotropic, and Lagrangian subspaces.
  2. Maurice A. de Gosson, Symplectic Geometry and Quantum Mechanics, Birkhäuser, 2006. DOI record. Relevant: Chapter 1, symplectic spaces and Lagrangian planes.