Contact covectors #
A covector a on a vector space V is contact for a bilinear form B when a ≠ 0 and B
restricts to a nondegenerate form on the hyperplane ker a
(Module.Dual.IsContact). This is the pointwise linear algebra of a contact form on a manifold:
a one-form α is contact exactly when, at every point x, the covector α_x is contact for the
bilinear form dα_x.
The condition only depends on B through its values on ker a × ker a
(Module.Dual.isContact_congr), and is unchanged when a or B is multiplied by a nonzero
scalar. Together these give the pointwise form of the rescaling law for contact forms: since
d(f α) = df ∧ α + f dα, and df ∧ α vanishes on ker α × ker α, the forms α and f α are
contact together whenever f vanishes nowhere.
For an alternating B, the hyperplane ker a carries a nondegenerate alternating form, so it has
even dimension and V has odd dimension (Module.Dual.IsContact.odd_finrank). A subspace of
ker a on which B vanishes has at most half the dimension of ker a, so 2 dim W + 1 ≤ dim V
(Module.Dual.IsContact.two_mul_finrank_add_one_le). This is the dimension bound for isotropic and
Legendrian submanifolds of a contact manifold.
Contact covectors arise on hyperplanes transverse to a vector. If B is nondegenerate and
alternating, L : U → V is injective and z is a vector outside the range of L which together
with it spans V, then u ↦ B z (L u) is contact for the restriction B (L ·) (L ·) of B to
U (Module.Dual.isContact_comp_compl₁₂). This is the pointwise reason why the primitive
ι_Z ω of a symplectic form restricts to a contact form on a hypersurface transverse to Z.
The symplectization form ((s, v), (t, w)) ↦ s * a w - t * a v + B v w on K × V
(Module.Dual.symplectizationForm) is nondegenerate exactly when a is contact for B
(Module.Dual.isContact_iff_nondegenerate_symplectizationForm). This is the pointwise linear
algebra of the symplectization: up to the factor eᵗ, it is the value of d(eᵗ α) at a point
(t, x) of ℝ × M, with a = α_x and B = dα_x.
For an alternating B and a contact covector a, the bilinear form B + a ⊗ a,
(v, w) ↦ B v w + a v * a w, is left-separating
(Module.Dual.IsContact.separatingLeft_add_smulRight), so in finite dimension v ↦ B v + a(v) a
is an isomorphism onto the dual. This is the pointwise contact flat map X ↦ ι_X dα + α(X) α of a
contact form. The preimage of a itself is characterized by the Reeb equations: B r + a(r) a = a
exactly when a r = 1 and B r = 0 (Module.Dual.IsContact.add_smulRight_apply_eq_self_iff).
A contact covector a on a finite-dimensional space has a Reeb vector r = a.reebVector B
(Module.Dual.reebVector): the unique vector with a r = 1 which is B-orthogonal to ker a.
For alternating B it spans the kernel of B, and V = ker a ⊕ K r. Replacing a by c a and
B by a form agreeing with c B up to a term l ∧ a changes r into c⁻¹ r plus an explicit
correction in ker a (Module.Dual.IsContact.reebVector_smul_eq_inv_smul_add_iff). This is the
pointwise form of the Reeb vector field of a contact form and of its rescaling law.
Main declarations #
Module.Dual.IsContact:a ≠ 0andBis nondegenerate onker a.Module.Dual.isContact_iff_of_isRefl: for a reflexiveB, the elementwise criterion: the only vector ofker awhich isB-orthogonal to all ofker ais zero.Module.Dual.isContact_congr,Module.Dual.isContact_smul_iff,Module.Dual.isContact_smul_bilinForm_iff: invariance under changes ofBoffker aand under nonzero rescaling ofaand ofB.Module.Dual.IsContact.even_finrank_ker,Module.Dual.IsContact.odd_finrank: the dimension count.Module.Dual.IsContact.two_mul_finrank_add_one_le: the dimension bound for subspaces ofker aon whichBvanishes.Module.Dual.isContact_comp_compl₁₂: the covectorB zrestricted to a hyperplane transverse tozis contact for the restriction of a nondegenerate alternatingB.Module.Dual.isContact_comp_linearEquiv_compl₁₂_iff,Module.Dual.IsContact.reebVector_comp_linearEquiv_compl₁₂: contactness and the Reeb vector are transported by linear equivalences.Module.Dual.symplectizationForm,Module.Dual.isContact_iff_nondegenerate_symplectizationForm: the symplectization form, which is nondegenerate exactly for contact covectors.Module.Dual.IsContact.separatingLeft_add_smulRight:B + a ⊗ ais left-separating.Module.Dual.IsContact.add_smulRight_apply_eq_self_iff: the preimage ofaunderv ↦ B v + a(v) a.Module.Dual.reebVector,Module.Dual.IsContact.eq_reebVector_iff: the Reeb vector and its characterization.Module.Dual.IsContact.ker_eq_span_reebVector,Module.Dual.IsContact.isCompl_ker_span_reebVector: the Reeb line is the kernel ofBand is complementary toker a.Module.Dual.IsContact.reebVector_smul_eq_inv_smul_add_iff: the rescaling law.
References #
- H. Geiges, An Introduction to Contact Topology, Cambridge University Press, 2008, Section 1.1.
A covector a is contact for a bilinear form B when it is nonzero and B restricts to a
nondegenerate bilinear form on the hyperplane ker a. For a one-form α on a manifold, the
covector α_x being contact for dα_x at every point x is the contact condition.
Instances For
A contact covector is nonzero.
A contact covector's bilinear form is nondegenerate on its kernel.
For a reflexive bilinear form, and in particular for an alternating one, a covector a is
contact exactly when it is nonzero and no nonzero vector of ker a is B-orthogonal to all of
ker a.
Whether a is contact for B only depends on the values of B on ker a × ker a.
A nonzero multiple of a covector is contact for B exactly when the covector is.
A covector is contact for a nonzero multiple of B exactly when it is contact for B.
For an alternating B, the kernel of a contact covector has even dimension.
A finite-dimensional space carrying a covector which is contact for an alternating bilinear form has odd dimension.
Isotropic subspaces of a contact hyperplane. If a is contact for B, then a subspace W
of ker a on which B vanishes identically satisfies 2 dim W + 1 ≤ dim V. No symmetry
assumption on B is needed.
Hyperplanes transverse to a vector #
Transverse hyperplanes of a nondegenerate alternating form carry contact covectors. Let
B be a nondegenerate alternating form on V, let L : U → V be injective, and let z be a
vector outside the range of L which together with it spans V, so that L identifies U with
a hyperplane transverse to z. Then the covector u ↦ B z (L u) on U is contact for the
restricted form B (L ·) (L ·).
This is the linear algebra behind hypersurfaces of contact type: when ι_Z ω = α for a vector
field Z transverse to a hypersurface, the restriction of α to the hypersurface is a contact
form.
Transport along linear equivalences #
Contactness is invariant under linear equivalences. For a linear equivalence
e : V ≃ V', the pullback a' ∘ e is contact for the pullback B' ∘ (e × e) exactly when a'
is contact for B'.
The symplectization form #
The symplectization form of a covector a and a bilinear form B on V: the bilinear
form ((s, v), (t, w)) ↦ s * a w - t * a v + B v w on K × V. Up to the positive factor eᵗ, it
is the value of d(eᵗ α) at a point (t, x) of ℝ × M, for a one-form α on a manifold M,
with a = α_x and B = dα_x.
Instances For
The symplectization form of an alternating form is alternating.
Swapping the arguments of the symplectization form of a and B gives the symplectization
form of -a and of the swapped form B.flip.
The symplectization form of a and B is left-separating exactly when a is nonzero and the
restriction of B to ker a is left-separating.
Symplectization of a contact covector. The symplectization form
((s, v), (t, w)) ↦ s * a w - t * a v + B v w on K × V is nondegenerate exactly when a is
contact for B. This is the pointwise reason why d(eᵗ α) is a symplectic form on ℝ × M
exactly when α is a contact form on M.
The contact flat map #
For an alternating B and a contact covector a, the bilinear form B + a ⊗ a,
(v, w) ↦ B v w + a v * a w, is left-separating. This is the linear algebra behind the
contact flat map v ↦ ι_v dα + α(v) α of a contact form, which is invertible in finite
dimension.
For an alternating B and a contact covector a, a vector r solves B r + a(r) a = a
exactly when a r = 1 and r is B-orthogonal to everything: these are the Reeb equations.
The Reeb vector #
The Reeb vector of a covector a for a bilinear form B: a vector r with a r = 1 which
is B-orthogonal to the hyperplane ker a, that is B r w = 0 whenever a w = 0. When a is
contact for B on a finite-dimensional space, there is exactly one such vector
(Module.Dual.IsContact.eq_reebVector_iff). If there is none, a.reebVector B is 0.
Instances For
The Reeb vector only depends on B through its values on V × ker a.
The Reeb vector does not change when B is multiplied by a nonzero scalar.
If a vector takes the value 1 under a and is B-orthogonal to ker a, the Reeb vector is
such a vector.
If no vector takes the value 1 under a while being B-orthogonal to ker a, the Reeb
vector is the junk value 0.
Rescaling a contact covector by a nonzero scalar c divides its Reeb vector by c. This holds
in every dimension: without a Reeb vector, both sides are the junk value 0.
Characterization of the Reeb vector. For a contact covector a, the Reeb vector is the
unique vector r with a r = 1 which is B-orthogonal to ker a.
A contact covector takes the value 1 on its Reeb vector.
The Reeb vector is B-orthogonal to the kernel of the contact covector.
The Reeb vector of a contact covector is nonzero.
The Reeb vector of a contact covector does not lie in its kernel.
The kernel of a contact covector and the line spanned by its Reeb vector are complementary:
V = ker a ⊕ K r.
The Reeb vector is transported by linear equivalences. If a' is contact for B',
then the Reeb vector of the pullback a' ∘ e for B' ∘ (e × e) is e⁻¹ of the Reeb vector of
a' for B'.
Rescaling law for the Reeb vector, pointwise. Let a be contact for B, let c ≠ 0,
and let B' be a bilinear form with B' v w = c B v w - l w a v for w ∈ ker a. This is the
situation of the contact form f α, where c = f x, l = df_x and B' = d(f α)_x. Then the Reeb
vector of c a for B' is c⁻¹ r + y, where r is the Reeb vector of a for B and y is the
unique vector of ker a with B y w = l w / c ^ 2 for all w ∈ ker a.
For an alternating B, the Reeb vector of a contact covector lies in the kernel of B:
B r w = 0 for every w, not only for w ∈ ker a.
For an alternating B, every vector is B-orthogonal to the Reeb vector from the left.
For an alternating B, the Reeb vector of a contact covector lies in the kernel of B.
For an alternating B, the Reeb vector of a contact covector is the unique vector r with
a r = 1 and B r = 0.
For an alternating B, the kernel of B is the line spanned by the Reeb vector of a contact
covector.