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Background. It is often said that two spaces are homeomorphic if, roughly speaking, one space can be continuously deformed into the other without any tearing and gluing. It is then emphasized that this is more of a guiding principle than a solid fact. Indeed, a well-known 'counterexample' to this heuristic would be double-twisted Möbius strip $M$, which is homeomorphic to the cylinder $C$, but when we visualize the two spaces in $\mathbb{R}^3$, we find that we cannot deform into each other without tearing.

Why does this happen? In a sense this is because $\mathbb{R}^3$ does not have enough room for the desired deformation; there simply aren't enough dimensions to 'untwist' the double twist without tearing things up. This leads us to the following:

Preliminary question. Suppose I were to embed $M$ and $C$ in $\mathbb{R}^n$ for some large $n$. Can I now deform one into the other without tearing or gluing?

The answer turns out to be yes, and in fact I believe $n = 4$ already suffices. If you care for the informal proof, read on; if not, scroll down to the main part. Let us start with a suitable embedding of a double twist.

enter image description here

This picture visualizes an embedding of the double twist within $\mathbb{R}^4$, where the first three dimensions are spatial, and the fourth dimension is represented by different colours. (The choice of colours may be unfortunate, but I did not have any other pens.) Now imagine moving the 'left strip' and the 'right strip' closer together, like so.

enter image description here

Notice that the 'double twist' starts to resemble a loop. Now, if we move the strips yet closer, they will start to overlap spatially. But notice that the colours will remain different on the overlap so that no actual tearing or gluing occurs. Now keep going until the two strips fully overlap each other. At this point the colors have aligned, so that the twist has turned into a 'loop'.

This loop is undesirable, but the solution to that issue is simple. During the proces in which we let the strips overlap, we simply let the size of the loop go to zero. At the very moment that the overlap is complete (and the colors have aligned), the size of the loop reaches, and as such the loop will vanish altogether. 'QED'.

To our main question. We see that our counterexample is no longer a counterexample. We might therefore wonder if this is part of a general phenomenon. Let us make this more precise.

Let $X$ be a topological space, and let $f : X\to \mathbb{R}^n$ and $g : X \to \mathbb{R}^n$ be two embeddings. Denote by $\varepsilon_{n,m} : \mathbb{R}^n \to \mathbb{R}^{n+m}$ the embedding which sends a point $x$ to $(x,0)$. Let's say $f$ can be deformed by embeddings into $g$ if there exists an $m$ and a homotopy from $H : X \times I \to \mathbb{R}^{n+m}$ from $\varepsilon_{n,m} \circ f$ to $\varepsilon_{n,m} \circ g$ such that for all $t\in [0,1]$, the map $H_t : X \to \mathbb{R}^{n+m}$ is a continuous embedding.

Question. Suppose $X$ is a reasonable space (say, a compact manifold with boundary). Let $f$ and $g$ be two embeddings of $X$ into some $\mathbb{R}^n$. Can $f$ always be deformed by embeddings into $g$?

This question can be generalized and specialized in many ways, so feel free to change some of its details.

  • Although this question has had an answer for a while, there is one issue which isn't discussed: the phrase "can be continuously deformed" is ambiguous. We are used to thinking about homotopies or isotopies when we hear that phrase. However, there is another meaning which is exactly correct: to say that "$X$ can be continuously deformed into $Y$ without any tearing or gluing" simply means that there is a function from $X$ to $Y$ which is continuous and injective (and surjective, and with a continuous inverse). – Lee Mosher Oct 17 '18 at 18:02
  • "Which is continuous and injective (and surjective, and with a continuous inverse)", well yes, but that is essentially by definition of 'homeomorphism', right? Or is there an immediate geometric idea behind this definition which I'm missing? – Sofie Verbeek Oct 17 '18 at 20:20
  • That's right. My point is that in a formal setting the word "deformation" is often a substitute for "homotopy" or "isotopy", but in an informal setting a phrase like "can be continuously deformed to" is often a substitute for "is homeomorphic to". – Lee Mosher Oct 17 '18 at 20:54

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Here's a theorem. Let $X$ be a closed subset of $\newcommand{\R}{\Bbb R}\R^m$ and $Y$ be a closed subset of $\R^n$. Let $X$ and $Y$ be homeomorphic. Embed $\R^m$ and $\R^n$ into $\R^{m+n}$ by $(x_1,\ldots,x_n)\mapsto (x_1,\ldots,x_m,0,\ldots,0)$ and $(y_1,\ldots,y_n)\mapsto (0,\ldots,0,y_1,\ldots,y_n)$. So we can think of $X$ and $Y$ as closed subsets of $\R^{m+n}$. Then the pairs $(\R^{m+n},X)$ and $(\R^{m+n},Y)$ are homeomorphic.

Let $f:X\to Y\subseteq\R^n$ be a homeomorphism. By Tietze's theorem, this extends to a continuous map $F:\R^m\to\R^n$. Now $(x,y)\mapsto(x,y+F(x))$ is a homeomorphism $\R^{m+n}\to\R^{m+n}$ taking $X$ to the graph $\Gamma$ of $f$. Therefore the pair $(\R^{m+n},X)$ is homeomorphic to $(\R^{m+n},\Gamma)$. Considering $f^{-1}:Y\to X$ instead gives $(\R^{m+n},Y)$ homeomorphic to $(\R^{m+n},\Gamma)$.

This homeomorphism $(\R^{m+n},X)\to(\R^{m+n},\Gamma)$ is part of a continuous family of homeomorphisms $(x,y)\mapsto(x,y+tF(x))$.

So the answer to your question is yes, for closed subsets of $\R^n$ and expanding the ambient Euclidean space to enough dimensions.

Angina Seng
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    Ah, I was already hoping that some general extension theorem could be invoked. Do you think there are methods to improve on the number of dimensions needed? For instance, in the example of my question, you need $4$ dimensions rather than $3 + 3 = 6$. – Sofie Verbeek Sep 15 '18 at 11:42