Darboux bases of a symplectic vector space #
Let ω be a symplectic form on a real vector space V. A Darboux basis of (V, ω)
(TauCeti.SymplecticForm.IsDarbouxBasis) is a basis (q₁, p₁, …, qₙ, pₙ), indexed by
Fin n × Fin 2 with qᵢ = b (i, 0) and pᵢ = b (i, 1), in which
ω(qᵢ, qⱼ) = 0, ω(pᵢ, pⱼ) = 0, ω(qᵢ, pⱼ) = δᵢⱼ,
so that ω = ∑ dqᵢ ∧ dpᵢ in the dual coordinates.
The relabelling TauCeti.SymplecticForm.darbouxIndexEquiv, (i, 0) ↦ inr i and
(i, 1) ↦ inl i, identifies Darboux bases with the bases in which the matrix of ω is Mathlib's
standard symplectic matrix Matrix.J
(TauCeti.SymplecticForm.isDarbouxBasis_iff_toMatrix_reindex, and conversely
TauCeti.SymplecticForm.isDarbouxBasis_reindex_symm_iff). Hence Darboux bases exist on a
finite-dimensional space (TauCeti.SymplecticForm.exists_isDarbouxBasis), and any two of them
have relative determinant 1 (TauCeti.SymplecticForm.IsDarbouxBasis.det_eq_one), from the
corresponding facts LinearMap.BilinForm.IsAlt.exists_basis_toMatrix_eq_J and
LinearMap.BilinForm.basis_det_eq_one_of_toMatrix_eq_J about nondegenerate alternating forms.
Every linear symplectomorphism of (V, ω) has determinant 1
(TauCeti.SymplecticForm.IsSymplectomorphism.det_eq_one), the specialization of
TauCeti.BilinForm.IsIsometry.det_eq_one_of_isAlt.
In a Darboux basis, pairing with the basis vectors reads off the coordinates of a vector:
ω(qᵢ, v) is its pᵢ-coordinate and ω(pᵢ, v) is minus its qᵢ-coordinate
(TauCeti.SymplecticForm.IsDarbouxBasis.apply_fst,
TauCeti.SymplecticForm.IsDarbouxBasis.apply_snd).
Darboux bases are carried to Darboux bases by linear symplectomorphisms
(TauCeti.SymplecticForm.IsDarbouxBasis.map), and the concatenation of Darboux bases of ω₁ and
ω₂ is a Darboux basis of the direct sum ω₁ ⊕ ω₂
(TauCeti.SymplecticForm.IsDarbouxBasis.prod).
Main definitions #
TauCeti.SymplecticForm.IsDarbouxBasis ω b:bis a Darboux basis of(V, ω).TauCeti.SymplecticForm.darbouxIndexEquiv n: the relabellingFin n × Fin 2 ≃ Fin n ⊕ Fin nbetween the Darboux and theMatrix.Jindex conventions.
References #
- D. McDuff and D. Salamon, Introduction to Symplectic Topology, 3rd ed., Oxford, 2017, Section 2.1 (symplectic bases).
- A. Cannas da Silva, Lectures on Symplectic Geometry, Lecture Notes in Mathematics 1764, Springer, 2001, Section 1.1.
A Darboux basis of a symplectic vector space (V, ω): a basis (q₁, p₁, …, qₙ, pₙ),
with qᵢ = b (i, 0) and pᵢ = b (i, 1), satisfying ω(qᵢ, qⱼ) = 0, ω(pᵢ, pⱼ) = 0 and
ω(qᵢ, pⱼ) = δᵢⱼ.
The vectors
qᵢpair trivially with each other.The vectors
pᵢpair trivially with each other.- apply_fst_snd (i j : Fin n) : (fun (v w : V) => (ω.toBilinForm v) w) (b (i, 0)) (b (j, 1)) = if i = j then 1 else 0
ω(qᵢ, pⱼ) = δᵢⱼ.
Instances For
In a Darboux basis, ω(pᵢ, qⱼ) = -δᵢⱼ.
In a Darboux basis, pairing with qᵢ reads off the pᵢ-coordinate:
ω(qᵢ, v) = b.repr v (i, 1).
In a Darboux basis, pairing with pᵢ reads off minus the qᵢ-coordinate:
ω(pᵢ, v) = -b.repr v (i, 0).
The relabelling (i, 0) ↦ inr i, (i, 1) ↦ inl i, under which a Darboux basis becomes a
basis in which ω has Mathlib's standard symplectic matrix Matrix.J
(TauCeti.SymplecticForm.isDarbouxBasis_iff_toMatrix_reindex).
Instances For
A basis is a Darboux basis exactly when, relabelled by darbouxIndexEquiv, it is a basis in
which the matrix of ω is Matrix.J.
A basis d indexed by Fin n ⊕ Fin n, relabelled by darbouxIndexEquiv, is a Darboux basis
exactly when the matrix of ω in d is Matrix.J.
Darboux bases exist: every finite-dimensional symplectic vector space has a Darboux basis.
A Darboux basis exists for any prescribed number n of pairs with finrank ℝ V = n * 2.
Darboux bases have unit relative determinant: the change of basis between two Darboux
bases of (V, ω) is a symplectic matrix, of determinant 1.
A linear symplectomorphism carries Darboux bases to Darboux bases.
Linear symplectomorphisms have determinant one. On an infinite-dimensional space the
determinant is 1 by convention.
Darboux bases of a direct sum. The concatenation of a Darboux basis b of ω₁ and a
Darboux basis c of ω₂, listing the pairs of b before those of c, is a Darboux basis of
ω₁ ⊕ ω₂.