The homotopy operator on a cylinder over a subset of a normed space #
Let ω : E × ℝ → (E × ℝ) [⋀^Fin (n + 1)]→L[ℝ] F be a differential (n + 1)-form on the product
of a real normed space E with the time line. The cylinder homotopy operator
(TauCeti.cylinderHomotopy) contracts ω with the unit time vector ∂ₜ = (0, 1) and integrates
the result over the time interval [0, 1]:
(h ω)(x)(v₁, …, vₙ) = ∫₀¹ ω(x, t)(∂ₜ, v₁, …, vₙ) dt,
where each vᵢ ∈ E is viewed in E × ℝ through ContinuousLinearMap.inl. Writing
ιₜ^* ω = x ↦ (ω (x, t)).compContinuousLinearMap (.inl ℝ E ℝ) for the pullback of ω along the
slice x ↦ (x, t), the operator satisfies the cochain-homotopy identity
d (h ω) + h (d ω) = ι₁^* ω - ι₀^* ω.
Everything is relative to a cylinder s ×ˢ Icc 0 1: the form only needs to be C¹ on it, and the
exterior derivatives are taken within it (and within s for h ω). The base s is a convex set
with unique derivatives that need not be open, such as a closed half-ball, the local shape of the
image of a boundary chart of a manifold with boundary; the time direction always has boundary.
Convexity is what Mathlib's mean value inequality needs to differentiate under the integral
within s. In degree zero the identity reduces to the fundamental theorem of calculus
h (d f) = ι₁^* f - ι₀^* f (TauCeti.cylinderHomotopy_extDerivWithin_eq_sub), which needs no
convexity.
The proof differentiates under the integral sign and uses the fundamental theorem of calculus in
the time variable. Pointwise, the derivative terms combine through the constant-coefficient Cartan
formula ContinuousAlternatingMap.alternatizeUncurryFin_curryLeft_comp_add_curryLeft for the
vector ∂ₜ, pulled back along inl by
ContinuousAlternatingMap.alternatizeUncurryFin_compContinuousLinearMap, into the time derivative
of ιₜ^* ω.
This is the chart-level form of the homotopy operator on forms on M × [0, 1] for a manifold M
with or without boundary, the analytic input for homotopy invariance of de Rham cohomology. It is
proved directly, without Stokes' theorem on the manifold with corners M × [0, 1].
Main declarations #
TauCeti.cylinderHomotopy: the cylinder homotopy operator.Convex.contDiffOn_cylinderHomotopy,TauCeti.contDiff_cylinderHomotopy: it preservesC^rregularity.Convex.extDerivWithin_cylinderHomotopy_add_cylinderHomotopy_extDerivWithin: the cochain-homotopy identityd (h ω) + h (d ω) = ι₁^* ω - ι₀^* ω.Convex.extDerivWithin_cylinderHomotopy: for a closed form,ι₁^* ω - ι₀^* ω = d (h ω).TauCeti.cylinderHomotopy_extDerivWithin_eq_sub: the degree-zero caseh (d f) = ι₁^* f - ι₀^* f.TauCeti.extDeriv_cylinderHomotopy_add_cylinderHomotopy_extDeriv,TauCeti.cylinderHomotopy_extDeriv_eq_sub: the same identities for formsC¹on all ofE × ℝ, with exterior derivatives on the whole spaces.TauCeti.support_cylinderHomotopy_subset,TauCeti.tsupport_cylinderHomotopy_subset,TauCeti.norm_cylinderHomotopy_le,TauCeti.norm_iteratedFDeriv_cylinderHomotopy_le: support and sup-norm bounds forh ωand its derivatives, which makehcontinuous on compactly supported smooth forms.
References #
- John M. Lee, Introduction to Smooth Manifolds, 2nd ed., Chapter 17, section Homotopy
Invariance, whose homotopy operator on
M × [0, 1]is the manifold version of this one. - R. Bott and L. W. Tu, Differential Forms in Algebraic Topology, GTM 82, §4 (the homotopy
operator
Kof the Poincaré lemma, integration along the fibre ofM × ℝ → M).
The cylinder homotopy operator: the n-form x ↦ ∫₀¹ ω(x, t)((0, 1), ·) dt on E built
from a differential (n + 1)-form ω on E × ℝ, with the arguments in E included into E × ℝ
by ContinuousLinearMap.inl. For a C¹ form with values in a Banach space it satisfies
d (h ω) + h (d ω) = ι₁^* ω - ι₀^* ω, where ιₜ is the slice x ↦ (x, t).
Instances For
The cylinder homotopy operator at x only depends on the form along the segment
{x} × [0, 1].
Evaluated on vectors v₁, …, vₙ of E, the cylinder homotopy operator is the time integral
∫₀¹ ω(x, t)(∂ₜ, (v₁, 0), …, (vₙ, 0)) dt, for a form integrable along the segment
{x} × [0, 1].
The cylinder homotopy operator of the zero form is zero.
The cylinder homotopy operator commutes with real scalar multiplication of forms.
The integrand t ↦ ω(x, t)(∂ₜ, (·, 0), …, (·, 0)) of the cylinder homotopy operator is
interval integrable for a form that is continuous along the segment {x} × [0, 1].
The cylinder homotopy operator is additive on forms that are continuous along the segment
{x} × [0, 1].
The cylinder homotopy operator is supported over the part of the support of the form that lies
in E × [0, 1].
The cylinder homotopy operator of a compactly supported form is topologically supported over
the part of the topological support of the form that lies in E × [0, 1].
The cylinder homotopy operator at x is bounded by any bound for the form along the segment
{x} × [0, 1], for the sup norm on E × ℝ.
The derivatives of the cylinder homotopy operator of a compactly supported C^r form are
bounded by those of the form: if ‖Dⁱ ω (x, t)‖ ≤ B for t ∈ [0, 1] and i ≤ r, then
‖Dⁱ (h ω) x‖ ≤ B, for the sup norm on E × ℝ.
The cylinder homotopy identity in degree zero, the fundamental theorem of calculus
h (d f) = ι₁^* f - ι₀^* f for a C¹ function f on the cylinder s ×ˢ Icc 0 1, viewed as a
0-form.
The cylinder homotopy operator of a form that is C^r on the cylinder s ×ˢ Icc 0 1 over a
convex set s with unique derivatives is C^r on s.
The cylinder homotopy identity d (h ω) + h (d ω) = ι₁^* ω - ι₀^* ω, with exterior
derivatives within s and within the cylinder s ×ˢ Icc 0 1, for a form C¹ on the cylinder
over a convex set s with unique derivatives. Here ιₜ^* ω is the pullback of ω along the
slice x ↦ (x, t).
Closed forms on a cylinder. For a form C¹ on the cylinder s ×ˢ Icc 0 1 over a convex
set s with unique derivatives and closed within the cylinder, the difference of its slice
pullbacks ι₁^* ω - ι₀^* ω is the exterior derivative within s of its cylinder homotopy
operator.
The cylinder homotopy operator of a form that is C^r on all of E × ℝ is C^r.
The cylinder homotopy identity d (h ω) + h (d ω) = ι₁^* ω - ι₀^* ω for a form that is
C¹ on all of E × ℝ, with exterior derivatives on the whole spaces. Here ιₜ^* ω is the
pullback of ω along the slice x ↦ (x, t).
The cylinder homotopy identity in degree zero, h (d f) = ι₁^* f - ι₀^* f for a function
f that is C¹ on all of E × ℝ, viewed as a 0-form.