Finding inverse for a homeomorphism on the sphere (compactification)

In summary: The sphere as a subset of Euclidean space inherits the Riemannian metric directly. You can do charts if you like but you need only to look at vectors in Euclidean space.
  • #1
huberscher
2
0
hi there

I'd like to show that the sphere
[tex]\mathbb{S}^n := \{ x \in \mathbb{R}^{n+1} : |x|=1 \}[/tex] is the one-point-compactification of [tex]\mathbb{R}^n[/tex] (*)

After a lot of trying I got this function:

[tex]f: \mathbb{S}^n \setminus \{(0,...,0,1)\} \rightarrow \mathbb{R}^n [/tex]
[tex](x_1,...,x_{n+1}) \mapsto (\frac{x_1}{1-x_{n+1}},...,\frac{x_n}{1-x_{n+1}}) [/tex]

This is a continuous function, its image is the whole [itex]\mathbb{R}^n[/itex]. If I find its inverse [itex]f^{-1} [/itex] now and show that this one is continuous as well with [itex]image(f^{-1})=\mathbb{S}^n \setminus \{(0,...,0,1)\}[/itex] I have shown (*).


But I don't find the inverse. [itex] y_i=\frac{x_i}{1-x_{n+1}} [/itex] so [itex] x_i=(1-x_{n+1})*y_1 [/itex] but there is no [itex]x_{n+1}[/itex] here y is a n-dimensional vector...?

How can I find the inverse of f?

Regards
 
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  • #2
first try solving for xn+1 in terms of x1,..xn.
 
  • #3
I don't get it:

If I consider the norms of those vectors I have with [itex] x=(x_1,...,x_n) [/itex]

[tex]\vec{x}*\frac{1}{1-x_{n+1}} =\vec{y} [/tex] so

[tex]x_{n+1}=\frac{\|y\|-\|x\|}{\|y\|} [/tex] but then I still have this y. What the trick here to get those [itex]x_{n+1}[/itex]?
 
  • #4
can you use the equation for the sphere to solve for xn+1 in terms on x1,..,xn?

start with case n=1.
 
  • #6
Steroegraphic projection is conformal so its inverse is also conformal. Is a congormal map continuous?

Is a conformal mapping an open mapping? That is, does it map open sets onto open sets?
If so, does that mean that its inverse is continuous?

This is to show you that you do not need to actually write down the inverse to check whether it is continuous. If you want write the inverse down think of solving for the intersection point on the sphere of straight line from a point in the plane to the north pole.
 
  • #7
lavinia said:
Steroegraphic projection is conformal so its inverse is also conformal. Is a congormal map continuous?

Is a conformal mapping an open mapping? That is, does it map open sets onto open sets?
If so, does that mean that its inverse is continuous?

This is to show you that you do not need to actually write down the inverse to check whether it is continuous. If you want write the inverse down think of solving for the intersection point on the sphere of straight line from a point in the plane to the north pole.

Still, you cannot treat a map into the Riemann sphere as you would a map from the

complex plane to itself. Even continuity is tricky, since the sphere is a manifold.

Or you can treat it as a map from C to C\/{oo}. And then the inverse function

theorem would tell you when the map is a homeomorphims/diffeomorphism.
 
  • #8
Bacle2 said:
Still, you cannot treat a map into the Riemann sphere as you would a map from the

complex plane to itself. Even continuity is tricky, since the sphere is a manifold.

Or you can treat it as a map from C to C\/{oo}. And then the inverse function

theorem would tell you when the map is a homeomorphims/diffeomorphism.

The sphere minus a point maps confomally onto the plane. Add the north pol and you compactify it.
 
  • #9
lavinia said:
The sphere minus a point maps confomally onto the plane. Add the north pol and you compactify it.

Yes, I know, this is what I said in post #7 . But conformality is usually defined for

maps from C to C , where there is a clear meaning of preservation of angles. If you

want to talk about preservation of angles for curves lying on the sphere, this is

a whole different story: do you use the tangent space of the sphere? How about

showing a map into the sphere into C is analytic (since conformal is equivalent to analytic

with non-zero derivative)? I'm not saying it is wrong; just that it needs an argument. What happens

with the image vectors near the north-pole? I don't see it; I may be wrong, but it does not seem automatic.

To talk about analytic in the sphere, you need to bring up charts.
 
Last edited:
  • #10
Bacle2 said:
Yes, I know, this is what I said in post #7 . But conformality is usually defined for

maps from C to C , where there is a clear meaning of preservation of angles. If you

want to talk about preservation of angles for curves lying on the sphere, this is

a whole different story: do you use the tangent space of the sphere? How about

showing a map into the sphere into C is analytic (since conformal is equivalent to analytic

with non-zero derivative)?

To talk about analytic in the sphere, you need to bring up charts.


The sphere as a subset of Euclidean space inherits the Riemannian metric directly. You can do charts if you like but you need only to look at vectors in Euclidean space.

But preserving infinitesimal angles in the plane is no different than on the sphere. Its just that the metrics are different.
 
  • #11
lavinia said:
The sphere as a subset of Euclidean space inherits the Riemannian metric directly. You can do charts if you like but you need only to look at vectors in Euclidean space.

But preserving infinitesimal angles in the plane is no different than on the sphere. Its just that the metrics are different.

Well, I think you would have to show/argue that the stereographic projection T as a map

from C to the sphere preserves the metric/inner-product in the sense that

<a,b>_C= <T(a),T(b)>_S^1 . I never saw this argument in your post.
 
  • #12
Moreover: if the stereo T preserved the metric: wouldn't this imply that C and S^1

are isometric?
 
  • #13
Bacle2 said:
Well, I think you would have to show/argue that the stereographic projection T as a map

from C to the sphere preserves the metric/inner-product in the sense that

<a,b>_C= <T(a),T(b)>_S^1 . I never saw this argument in your post.

the metric isn't preserved but the map is conformal, angles are preserved infinitesimally. The same thing is true for analytic maps of the complex plane.
I am beginning to think that I misunderstood your point. i am sorry if I did.
 
  • #14
lavinia said:
the metric isn't preserved but the map is conformal, angles are preserved infinitesimally. The same thing is true for analytic maps of the complex plane.
I am beginning to think that I misunderstood your point. i am sorry if I did.

No problem; you may be right and we may be talking about different things. I think it may take too long to untangle ; I think it's run its course.
 

Related to Finding inverse for a homeomorphism on the sphere (compactification)

1. What is a homeomorphism on the sphere?

A homeomorphism on the sphere is a continuous function that maps points on a sphere to other points on the same sphere while preserving the topological properties of the sphere. In other words, a homeomorphism on the sphere is a one-to-one and onto mapping that does not create any holes, tears, or self-intersections on the surface of the sphere.

2. What is the inverse of a homeomorphism on the sphere?

The inverse of a homeomorphism on the sphere is a function that reverses the mapping of the original homeomorphism. It maps points on the sphere back to their original positions before the homeomorphism was applied.

3. Why is finding the inverse for a homeomorphism on the sphere important?

Finding the inverse for a homeomorphism on the sphere is important because it allows us to undo any transformations that were applied to the sphere using the original homeomorphism. This is useful in many mathematical and scientific applications, such as geometry, topology, and computer graphics.

4. How do you find the inverse for a homeomorphism on the sphere?

To find the inverse for a homeomorphism on the sphere, you can use a variety of mathematical techniques such as algebraic manipulation, geometric constructions, or numerical methods. The exact method used will depend on the specific homeomorphism and its properties.

5. What is the compactification of a sphere?

The compactification of a sphere is the process of adding a point at infinity to a sphere, resulting in a compact topological space. This point at infinity is known as the "one-point compactification" and allows for the inclusion of points that were previously unreachable in the original sphere. Compactification is often used in topology and differential geometry to simplify calculations and proofs.

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