The isotopy extension theorem #
Let F be a smooth isotopy from f₀ to f₁, a jointly smooth motion of a boundaryless manifold
M through smooth embeddings into a finite-dimensional boundaryless manifold N. On every compact
subset A of M, the motion is the restriction of a compactly supported diffeotopy of N
(TauCeti.SmoothIsotopy.exists_diffeotopy_apply_eq): there is a diffeotopy Φ, fixing every
point outside a compact set, with Φ (t, f₀ x) = F (σ t, x) for x ∈ A, where σ is the smooth
change of time Real.smoothTransition. In particular its final diffeomorphism carries f₀ to f₁
on A (TauCeti.SmoothIsotopy.exists_diffeotopy_final_apply_eq). This is the isotopy extension
theorem of Hirsch, Chapter 8, Theorem 1.3, for compact parts of the source; the source itself need
not be compact. The diffeotopy can moreover be chosen to fix a closed set C which the moving part
of A never meets (TauCeti.SmoothIsotopy.exists_diffeotopy_apply_eq_of_forall_notMem): the
ambient velocity field is cut off by a smooth function equal to 1 on the motion of that part and
to 0 on C.
The proof integrates a velocity field. Run at the time σ s, the motion of A is stationary for
s ≤ 0 and s ≥ 1, and TauCeti.SmoothIsotopy.exists_ambientVelocityField extends its velocity
to a time-dependent vector field X on N vanishing outside a fixed compact set K. Such a field
has a complete suspension (TauCeti.isCompleteVectorField_timeDependentSuspensionField), so its
time-dependent flow from time 0 is a diffeotopy (TauCeti.timeDependentFlowDiffeotopy), fixing
the complement of K. For x ∈ A, the curve s ↦ F (σ s, x) solves the time-dependent equation
of X and starts at f₀ x, so by uniqueness of solutions
(TauCeti.timeDependentFlowOf_eq_of_hasMFDerivAt) it is the flow line of f₀ x. The velocity
field loses one derivative: a C^n isotopy, 2 ≤ n, gives a C^m diffeotopy for every m with
1 ≤ m and m + 1 ≤ n, and a smooth isotopy a smooth diffeotopy.
For a compact source, smooth isotopy and smooth ambient isotopy of smooth embeddings are therefore
the same relation (TauCeti.smoothAmbientIsotopic_iff_smoothIsotopic); the forward implication is
TauCeti.SmoothAmbientIsotopic.smoothIsotopic.
Main results #
TauCeti.SmoothIsotopy.exists_diffeotopy_apply_eq: a smooth isotopy is, on a compact subset of its source, the restriction of a compactly supported diffeotopy, after the change of timeReal.smoothTransition.TauCeti.SmoothIsotopy.exists_diffeotopy_apply_eq_of_forall_notMem: the same, with the diffeotopy fixing a closed set missed by the moving part of the compact subset.TauCeti.SmoothIsotopy.exists_diffeotopy_final_apply_eq: the final diffeomorphism of that diffeotopy carries the initial embedding to the final one on the compact subset.TauCeti.SmoothIsotopic.smoothAmbientIsotopic: smoothly isotopic smooth maps of a compact boundaryless manifold are smoothly ambient isotopic.TauCeti.smoothAmbientIsotopic_iff_smoothIsotopic: for smooth embeddings of a compact boundaryless manifold, smooth ambient isotopy is smooth isotopy.
References #
- M. W. Hirsch, Differential Topology, Graduate Texts in Mathematics 33, Springer (1976), Chapter 8, §1, Theorems 1.3 and 1.4.
Isotopy extension fixing a closed set. Let F be a C^n isotopy through smooth embeddings
into a finite-dimensional boundaryless manifold, and A, A₀ compact subsets of the source such
that F keeps fixed every point of A outside A₀. If the motion of A₀ never
meets the closed set C, then the motion of A is the restriction of a C^m diffeotopy Φ of
the target fixing every point of C and every point outside a compact set, for 1 ≤ m and
m + 1 ≤ n: Φ (t, f₀ x) = F (σ t, x) for x ∈ A, where σ is the change of time
Real.smoothTransition, and Φ (t, y) = y for y ∈ C.
This is how isotopy extension leaves alone a part of the target that the isotopy does not move, such as the rest of a line along which an arc is straightened.
Isotopy extension on a compact subset. A C^n isotopy F of a boundaryless manifold
through smooth embeddings into a finite-dimensional boundaryless manifold is, on any compact subset
A of the source, the restriction of a C^m diffeotopy Φ of the target fixing every point
outside a compact set, for 1 ≤ m and m + 1 ≤ n: Φ (t, f₀ x) = F (σ t, x) for x ∈ A, where
σ t = Real.smoothTransition t. The source need not be compact.
Isotopy extension on a compact subset, final form. The final diffeomorphism of a compactly
supported C^m diffeotopy carries the initial embedding f₀ of a C^n isotopy to the final one
f₁ on any compact subset of the source, for 1 ≤ m and m + 1 ≤ n.
Smooth isotopy implies smooth ambient isotopy for a compact source. Smoothly isotopic smooth maps of a compact boundaryless manifold into a finite-dimensional boundaryless manifold are smoothly ambient isotopic.
Smooth ambient isotopy is smooth isotopy for a compact source. A smooth embedding f₀ of a
compact boundaryless manifold into a finite-dimensional boundaryless manifold is smoothly ambient
isotopic to a smooth map f₁ exactly when it is smoothly isotopic to it.