2024-07-29

706: For Half Euclidean \(C^\infty\) Manifold with Boundary, Open Half Ball Is Diffeomorphic to Whole Space

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description/proof of that for half Euclidean \(C^\infty\) manifold with boundary, open half ball is diffeomorphic to whole space

Topics


About: \(C^\infty\) manifold

The table of contents of this article


Starting Context



Target Context


  • The reader will have a description and a proof of the proposition that for any half Euclidean \(C^\infty\) manifold with boundary, any open half ball is diffeomorphic to the whole space.

Orientation


There is a list of definitions discussed so far in this site.

There is a list of propositions discussed so far in this site.


Main Body


1: Structured Description


Here is the rules of Structured Description.

Entities:
\(\mathbb{H}^d\): \(= \text{ the Euclidean } C^\infty \text{ manifold with boundary }\)
\(p\): \(\in Bou (\mathbb{H}^d)\), where \(Bou (\mathbb{H}^d)\) denotes the manifold boundary of \(\mathbb{H}^d\)
\(H_{p, \epsilon}\): \(= \text{ the open half ball around } p \text{ on } \mathbb{H}^d\)
\(g\): \(: H_{p, \epsilon} \to \mathbb{H}^d, p' \mapsto (p' - p) / \sqrt{\epsilon^2 - \Vert p' - p \Vert^2}\)
//

Statements:
\(H_{p, \epsilon} \cong_g \mathbb{H}^d\), where \(\cong_g\) denotes being diffeomorphic by \(g\)
//


2: Natural Language Description


For the half Euclidean \(C^\infty\) manifold with boundary, \(\mathbb{H}^d\), any open half ball around any \(p \in Bou (\mathbb{H}^d)\), where \(Bou (\mathbb{H}^d)\) denotes the manifold boundary of \(\mathbb{H}^d\), \(H_{p, \epsilon} \subseteq \mathbb{H}^d\) is diffeomorphic to \(\mathbb{H}^d\) by \(g: H_{p, \epsilon} \to \mathbb{H}^d, p' \mapsto (p' - p) / \sqrt{\epsilon^2 - \Vert p' - p \Vert^2}\).


3: Proof


Whole Strategy: Step 1: see that \(g\) is a restriction of \(f\) cited in the proposition that for any Euclidean \(C^\infty\) manifold, any open ball is diffeomorphic to the whole space; Step 2: take the identity chart on \(\mathbb{H}^d\), \((\mathbb{H}^d \subseteq \mathbb{H}^d, id)\); Step 3: see that \(id \circ g \circ id^{-1} \vert_{id (H_{p, \epsilon})}: id (H_{p, \epsilon}) \to id (\mathbb{H}^d)\) has the \(C^\infty\) extension, \(f: B_{p, \epsilon} \to \mathbb{R}^d\); Step 4: see that \(id \circ g^{-1} id^{-1}: id (\mathbb{H}^d) \to id (\mathbb{H}^d)\) has the \(C^\infty\) extension, \(f^{-1}: \mathbb{R}^d \to \mathbb{R}^d\).

Step 1:

\(g\) is in fact a restriction of \(f\) cited in the proposition that for any Euclidean \(C^\infty\) manifold, any open ball is diffeomorphic to the whole space.

That implies that \(g\) is injective; the surjectiveness is obvious: while the \(d\)-th component of \(p\) is zero, for each \(p'' \in \mathbb{H}^d\), there is a \(p' \in B_{p, \epsilon}\) such that \(f (p') = p''\), but as the \(d\)-th component of \(p''\) is non-negative, the \(d\)-th component of \(p'\) is non-negative, which means that \(p' \in H_{p, \epsilon}\).

So, there is the inverse, \(g^{-1}: \mathbb{H}^d \to H_{p, \epsilon}\).

Step 2:

Let us take the identity chart, \((\mathbb{H}^d \subseteq \mathbb{H}^d, id)\).

Step 3:

\(C^\infty\)-ness of \(g\) is about whether \(id \circ g \circ id^{-1} \vert_{id (H_{p, \epsilon})}: id (H_{p, \epsilon}) \to id (\mathbb{H}^d)\) has a \(C^\infty\) extension, according to the definition of map between arbitrary subsets of \(C^\infty\) manifolds with boundary \(C^k\) at point, where \(k\) excludes \(0\) and includes \(\infty\). But \(f: B_{p, \epsilon} \to \mathbb{R}^d\) is indeed such an extension.

So, \(g\) is \(C^\infty\).

Step 4:

\(C^\infty\)-ness of \(g^{-1}\) is about whether \(id \circ g^{-1} \circ id^{-1}: id (\mathbb{H}^d) \to id (\mathbb{H}^d)\) has a \(C^\infty\) extension, according to the definition of map between arbitrary subsets of \(C^\infty\) manifolds with boundary \(C^k\) at point, where \(k\) excludes \(0\) and includes \(\infty\). But \(f^{-1}: \mathbb{R}^d \to \mathbb{R}^d\) is indeed such an extension: \(f^{-1}\) is really \(f^{-1}: \mathbb{R}^d \to B_{p, \epsilon}\), but the codomain can be expanded without any harm.

So, \(g^{-1}\) is \(C^\infty\).


References


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