symplectic form - definição. O que é symplectic form. Significado, conceito
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O que (quem) é symplectic form - definição

VECTOR SPACE EQUIPPED WITH AN ALTERNATING NONDEGENERATE BILINEAR FORM
Symplectic form; Linear symplectic space; Lagrangian subspace; Symplectic product; Symplectic algebra; Symplectic bilinear form; Symplectic complement

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.
Tautological one-form         
CANONICAL DIFFERENTIAL FORM DEFINED ON THE COTANGENT BUNDLE OF A SMOOTH MANIFOLD
Symplectic potential; Liouville one-form; Canonical one form; Canonical one-form; Canonical 1-form; Canonical symplectic form; Liouville form; Poincaré one-form; Poincaré two-form; Poincaré 2-form; Poincaré 1-form; Poincare one-form
In mathematics, the tautological one-form is a special 1-form defined on the cotangent bundle T^{*}Q of a manifold Q. In physics, it is used to create a correspondence between the velocity of a point in a mechanical system and its momentum, thus providing a bridge between Lagrangian mechanics with Hamiltonian mechanics (on the manifold Q).
Symplectic geometry         
BRANCH OF DIFFERENTIAL GEOMETRY AND DIFFERENTIAL TOPOLOGY
Symplectic Geometry; Symplectic structure; Symplectic topology
Symplectic geometry is a branch of differential geometry and differential topology that studies symplectic manifolds; that is, differentiable manifolds equipped with a closed, nondegenerate 2-form. Symplectic geometry was founded by the Russian mathematician Vladimir Arnold and has its origins in the Hamiltonian formulation of classical mechanics where the phase space of certain classical systems takes on the structure of a symplectic manifold.

Wikipédia

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 ω : V × VF that is

Bilinear
Linear in each argument separately;
Alternating
ω(v, v) = 0 holds for all vV; and
Non-degenerate
ω(u, v) = 0 for all vV implies that u = 0.

If the underlying field has characteristic not 2, alternation is equivalent to skew-symmetry. If the characteristic is 2, the skew-symmetry is implied by, but does not imply alternation. In this case every symplectic form is a symmetric form, but not vice versa.

Working in a fixed basis, ω can be represented by a matrix. The conditions above are equivalent to this matrix being skew-symmetric, nonsingular, and hollow (all diagonal entries are zero). This should not be confused with a symplectic matrix, which represents a symplectic transformation of the space. If V is finite-dimensional, then its dimension must necessarily be even since every skew-symmetric, hollow matrix of odd size has determinant zero. Notice that the condition that the matrix be hollow is not redundant if the characteristic of the field is 2. A symplectic form behaves quite differently from a symmetric form, for example, the scalar product on Euclidean vector spaces.