The linear normal form of a contact covector #
On Kⁿ × Kⁿ × K, with coordinates (q, p, z), the standard contact covector is dz
(TauCeti.stdContactCovector) and the standard contact bilinear form is Σᵢ dqᵢ ∧ dpᵢ,
((q, p, z), (q', p', z')) ↦ q ⬝ᵥ p' - p ⬝ᵥ q' (TauCeti.stdContactBilinForm). These are the
values at the origin of the standard contact form dz - Σᵢ pᵢ dqᵢ and of its exterior derivative.
The standard covector is contact for the standard form
(TauCeti.isContact_stdContactCovector), with Reeb vector ∂_z = (0, 0, 1)
(TauCeti.reebVector_stdContactCovector).
This file proves that every contact covector is standard in suitable linear coordinates. If a is
contact for an alternating form B on a finite-dimensional space V, there is a linear
equivalence e : V ≃ Kⁿ × Kⁿ × K with a = dz ∘ e and B = (Σᵢ dqᵢ ∧ dpᵢ) ∘ (e × e)
(Module.Dual.IsContact.exists_linearEquiv_eq_stdContact). Conversely such coordinates make
a contact for B (Module.Dual.isContact_iff_exists_linearEquiv_eq_stdContact). Consequently
any two contact covectors for alternating forms on spaces of the same dimension are carried to each
other by a linear equivalence that also carries one form to the other
(Module.Dual.IsContact.exists_linearEquiv_of_finrank_eq).
The coordinates are built from the splitting V = ker a ⊕ K r along the Reeb vector r, and a
symplectic basis of the nondegenerate alternating form that B restricts to on ker a
(LinearMap.BilinForm.IsAlt.exists_basis_toMatrix_eq_J). They map the Reeb vector to ∂_z, as
both contactness and the Reeb vector are transported by linear equivalences
(Module.Dual.isContact_comp_linearEquiv_compl₁₂_iff,
Module.Dual.IsContact.reebVector_comp_linearEquiv_compl₁₂).
This is the pointwise normal form underlying the contact Darboux theorem: at a point of a contact manifold, the contact form and its exterior derivative take the standard values in a suitable basis of the tangent space.
References #
- H. Geiges, An Introduction to Contact Topology, Cambridge University Press, 2008, Section 2.5 (the linear algebra behind the contact Darboux theorem).
The standard contact covector dz on Kⁿ × Kⁿ × K, with coordinates (q, p, z). It is
the value at the origin of the standard contact form dz - Σᵢ pᵢ dqᵢ.
Instances For
The standard contact bilinear form Σᵢ dqᵢ ∧ dpᵢ on Kⁿ × Kⁿ × K, with coordinates
(q, p, z): ((q, p, z), (q', p', z')) ↦ q ⬝ᵥ p' - p ⬝ᵥ q'. It is the exterior derivative of the
standard contact form dz - Σᵢ pᵢ dqᵢ.
Instances For
The standard contact bilinear form is alternating.
The standard contact covector dz is contact for the standard bilinear form
Σᵢ dqᵢ ∧ dpᵢ.
The Reeb vector of the standard contact covector is ∂_z = (0, 0, 1).
The normal form #
Linear normal form of a contact covector. If a is contact for an alternating form B on
a finite-dimensional space V, there are linear coordinates e : V ≃ Kⁿ × Kⁿ × K in which a is
the standard contact covector dz and B is the standard form Σᵢ dqᵢ ∧ dpᵢ. Such coordinates
send the Reeb vector of a to ∂_z (Module.Dual.IsContact.reebVector_comp_linearEquiv_compl₁₂,
TauCeti.reebVector_stdContactCovector).
Contact covectors are those with standard linear coordinates. For an alternating form B
on a finite-dimensional space, a is contact for B exactly when some linear coordinates
e : V ≃ Kⁿ × Kⁿ × K make a the standard covector dz and B the standard form
Σᵢ dqᵢ ∧ dpᵢ.
Uniqueness of linear contact structures. Two contact covectors for alternating forms, on finite-dimensional spaces of the same dimension, are carried to each other by a linear equivalence which also carries one form to the other.