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The velocity field of an isotopy is well defined along its image

Statement

Let M be a compact smooth manifold, let N be a smooth manifold and let F:M×I→N be a smooth isotopy of embeddings with track F‾ and S:=F‾(M×I)⊆N×I (Smooth isotopies, diffeotopies and ambient isotopies). Then:

  1. F‾ is a smooth embedding and its image S is closed and diffeomorphic to M×I. Here embedding and diffeomorphism use the local coordinate-extension convention of the isotopy definition. The domain M×I has product corners at ∂M×{0,1} when M has boundary, and S carries the corresponding embedded track charts. If ∂M=∅, only the time-endpoint boundary faces occur. No neatness relative to the boundary faces of N×I is asserted.
  2. The horizontal velocity Y, well defined by Y(F(x,t),t):=dF(x,t)(0,∂t)∈TF(x,t)N⊆T(F(x,t),t)(N×I), is a smooth horizontal field along S: its pullback by F‾ is smooth up to the time endpoints, it takes values in the subbundle TN⊕0, and it satisfies dF‾(x,t)(∂t)=(Y(F‾(x,t)),∂t).
  3. If F takes values in ∂N, then Y takes values in the subbundle T(∂N); if F takes values in the interior of N, then so does the base point of Y.

No orientation, properness or injectivity beyond that of the isotopy is used, and no choice principle is needed.

Facts & Assumptions

Given: A compact smooth manifold M, a smooth manifold N, a smooth isotopy of embeddings F:M×I→N, its track F‾ and the set S=F‾(M×I).

[F1]

F is smooth, each slice Ft is a smooth embedding, and F‾(x,t)=(F(x,t),t); the horizontal velocity is defined by the displayed formula, ∂t denoting the standard unit tangent vector on the I factor (Smooth isotopies, diffeotopies and ambient isotopies, The differential of a smooth map).

[F2]

A smooth embedding is an injective immersion and a homeomorphism onto its image with the subspace topology (Smooth embeddings); a tangent vector in T(x,t)(M×I) is a pair of components in TxM and TtI (The tangent bundle as a disjoint union).

[L2]

The boundaryless embedding-image and product results do not themselves apply at t=0,1. Smoothness at source boundary faces and time endpoints means local smooth extension of coordinate functions across these faces (Smooth maps between manifolds with boundary). The local inverse needed here is established in step 2.2 using The smooth inverse function theorem on manifolds.

[L4]

Use product coordinates (u,t) on M×I, with smooth local extensions across source boundary faces and time endpoints. Smoothness and product differentials are computed componentwise in these coordinates, exactly as for the boundaryless product results (Products of smooth manifolds have a canonical product smooth structure, A map into a product is smooth iff its components are smooth).

[L5]

For smooth G,H one has d(H∘G)p=dHG(p)∘dGp (The chain rule for differentials of smooth maps), and the diagonal entry of a product differential is computed componentwise. Smooth maps are continuous (Smooth maps are continuous).

[L7]

In a boundary chart of N the boundary stratum is the coordinate hyperplane of last coordinate 0 and the interior is the open half-space of last coordinate >0 (Interior and boundary of a manifold with boundary, Smooth maps between manifolds with boundary).

Proof

technique · direct
1.1F1F2L4

The track F‾ is smooth by [L4], its two components being F and the projection M×I→I, which are smooth. It is injective: if F‾(x,t)=F‾(x′,t′) then reading the second coordinate gives t=t′ and the first gives Ft(x)=Ft(x′), so x=x′ because Ft is injective by [F2].

1.2F1F2L5

The track is an immersion. Let (v,a)∈TxM⊕TtI satisfy dF‾(x,t)(v,a)=0. Applying dπI and [L5] to πI∘F‾=prI gives a=0; then applying dπN to πN∘F‾=F gives d(Ft)x(v)=0, so v=0 because Ft is an immersion. Hence dF‾(x,t) is injective for every (x,t).

2.1L5L6step 1.1

The track is proper: M×I is compact by [L6] and F‾ is continuous by [F1] and [L5]. For a compact K⊆N×I, the target being Hausdorff by [L6], K is closed, so F‾−1(K) is closed in the compact space M×I and hence compact by [L6].

2.2L2L6step 1.1step 1.2construct

A continuous injective map from the compact space M×I into the Hausdorff space N×I is a homeomorphism onto its image: it sends closed sets to compact, hence closed, sets by [L6]. With step 1.2 this makes the track an embedding. For its smooth inverse, choose source coordinates u in a Euclidean open set or half-space of dimension dim⁡M and target coordinates y near one track point. Select dim⁡M target components p(y) for which Du(p∘F) is invertible. The map (u,t)↦(p(F(u,t)),t) has invertible block differential. Locally extend its coordinate functions across any source boundary face and time endpoint and apply [L2]'s inverse function theorem in Euclidean open sets. Its smooth inverse recovers (u,t) from (p(y),t) along the track. The other target components are smooth functions of these coordinates, giving the local graph model and the smooth inverse on S, including its source boundary and endpoint faces and their intersections. If N has boundary, extend its coordinate functions in Euclidean space for this calculation and then restrict back; no neatness or boundaryless slice theorem is invoked. Finally S is compact and therefore closed by [L6].

3.1F2step 1.1step 2.2

The velocity Y is well defined: a point of S has the form F‾(x,t) for a unique (x,t), because F‾ is injective by step 1.1, so the prescription Y(F‾(x,t)):=dF(x,t)(0,∂t) is independent of choices; this value lies in TF(x,t)N seen inside T(F(x,t),t)(N×I) by [F2].

4.1L2L4step 2.2step 3.1

On S one has Y=V∘F‾−1, where V(x,t):=dF(x,t)(0,∂t). The inverse is smooth in the local graph coordinates of step 2.2. The target components of V are time partial derivatives of the coordinate functions of F, hence are smooth, including at product corners by differentiating their local extensions. Thus Y is smooth along S in the stated local-extension sense.

4.2L5F1step 3.1

The tangent identity dF‾(x,t)(∂t)=(Y(F‾(x,t)),∂t) holds: by [L5] applied to the two components πN∘F‾=F and πI∘F‾=prI, the first component of dF‾(x,t)(∂t) is dF(x,t)(0,∂t)=Y(F‾(x,t)) and the second is dprI(∂t)=∂t.

5.1step 3.1step 4.1step 4.2

Consequently Y is a smooth field along the closed track, takes values in TN⊕0 by construction, and satisfies the tangent identity of step 4.2; this is clause 2.

6.1F1L7step 3.1∎

Assume F takes values in ∂N. Fix (x,t)∈M×I and a boundary chart of N at F(x,t) with last coordinate un; by [L7] the last coordinate of the curve s↦F(x,s) is identically 0 near s=t, so its derivative, which is the TN-component Y(F‾(x,t)) of the velocity, has last coordinate 0 and therefore lies in T(∂N). If instead F takes values in the interior of N, then the base point F(x,t) of Y(F‾(x,t)) lies in the interior by hypothesis. This is clause 3.

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