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Finite constrained mode quotient
Statement
Let be a finite-dimensional real vector space with a nondegenerate alternating bilinear form . For a linear subspace , define , and assume (so is coisotropic). Then the quotient vector space , whose elements are cosets , carries the well-defined symplectic form . This proposition concerns only finite-dimensional constrained mode models; it does not assert that an infinite-dimensional Einstein–Maxwell solution space has a smooth symplectic quotient.
Statement references
Facts & Assumptions
Given: A finite-dimensional real symplectic vector space and a linear subspace with .
Isotropic, coisotropic, symplectic, and Lagrangian subspaces: coisotropic means , where .
Symplectic reduction of a coisotropic vector subspace: for a symplectic vector space and coisotropic subspace , has the well-defined nondegenerate alternating form .
Proof
The hypothesis is exactly the coisotropic condition in [F1]. Thus the quotient and descended form in [F2] apply to this .
By [F2], changing either representative by an element of leaves unchanged, and a class in the radical has representative in , so the descended form is well-defined and nondegenerate. It is alternating by the alternation of . Since is a subspace of finite-dimensional , is finite-dimensional, so it is a finite-dimensional symplectic vector space. No infinite-dimensional quotient regularity is used.
Remarks
For the quotient is itself; for a Lagrangian constraint subspace the quotient is the zero symplectic vector space. These are finite-dimensional boundary cases of the stated result, not evidence for an infinite-dimensional solution-space reduction.