Homotopy between identity and antipodal map

  • Thread starter Thread starter jgens
  • Start date Start date
  • Tags Tags
    Identity Map
Click For Summary
SUMMARY

The discussion centers on proving that the identity map \(\mathrm{id}_{S^{2k+1}}\) and the antipodal map \(-\mathrm{id}_{S^{2k+1}}\) are smoothly homotopic. The proposed solution involves defining a smooth map \(h: S^{2k+1} \times \mathbb{R} \rightarrow S^{2k+1}\) that transitions from the identity to the antipodal map through a rotation parameterized by \(t\). The proof is completed by demonstrating that \(h\) is smooth, leveraging the smoothness of the mapping \(H: \mathbb{R}^{2k+2} \times \mathbb{R} \rightarrow \mathbb{R}^{2k+2}\). The necessity of including atlases for manifolds in the proof is debated, with the conclusion that they may be superfluous.

PREREQUISITES
  • Understanding of smooth manifolds and smooth maps
  • Familiarity with homotopy theory in topology
  • Knowledge of the standard basis in \(\mathbb{R}^{2k+2}\)
  • Concept of local representations and smooth atlases
NEXT STEPS
  • Study the properties of smooth maps in topology
  • Learn about homotopy equivalences and their applications
  • Explore the concept of smooth atlases in differential geometry
  • Investigate the implications of the antipodal map in higher-dimensional spheres
USEFUL FOR

Mathematicians, particularly those specializing in topology and differential geometry, as well as students tackling advanced concepts in smooth manifolds and homotopy theory.

jgens
Gold Member
Messages
1,575
Reaction score
50

Homework Statement



Prove that the identity map \mathrm{id}_{S^{2k+1}} and the antipodal map -\mathrm{id}_{S^{2k+1}} are smoothly homotopic.

Homework Equations



N/A

The Attempt at a Solution



My attempt:
Fix k \in \mathbb{Z}_{\geq 0} and let \{e_i\}_{i=1}^{2k+2} be the standard basis for \mathbb{R}^{2k+2}. Define the map h:S^{2k+1} \times \mathbb{R} \rightarrow S^{2k+1} by setting
<br /> h:\left(\sum_{i=1}^{2k+2}x_ie_i,t\right) \mapsto \sum_{i=1}^{k+1}\left(x_{2i-1}\cos{\pi t}-x_{2i}\sin{\pi t}\right)e_{2i-1} + \sum_{i=1}^{k+1}\left(x_{2i-1}\sin{\pi t}+x_{2i}\cos{\pi t}\right)e_{2i}<br />
This map satisfies h(x,0) = x and h(x,1) = -x. To complete the proof it only needs to be shown that h is a smooth map.

Let B^{2k+1} denote the open unit ball in \mathbb{R}^{2k+1} and for each i \in \{1,\dots,2k+2\} define the open hemispheres U_i^{\pm} = \{(x_1,\dots,x_{2k+2}) \in S^{2k+1}:\mathrm{sgn}(x_i) = \pm 1\}. Define for each i \in \{1,\dots,2k+2\} the maps \phi_i^{\pm}:U_i^{\pm} \rightarrow B^{2k+1} such that (x_1,\dots,x_{2k+2}) \mapsto (x_1,\dots,\hat{x_i},\dots,x_{2k+2}). Then the collection \{(U_i^{\pm},\phi_i^{\pm})\} is a smooth atlas for S^{2k+1} and the collection \{(U_i^{\pm} \times \mathbb{R},\phi_i^{\pm} \times \mathrm{id}_{\mathbb{R}})\} is a smooth atlas for S^{2k+1} \times \mathbb{R}. Notice that for each i \in \{1,\dots,2k+2\} a simple computation show that the local representation \phi_i^{\pm} \circ h \circ (\phi_i^{\pm} \times \mathrm{id}_{\mathbb{R}})^{-1} is smooth. This establishes that h is a smooth map and completes the proof.My comments:
So obviously there a some details missing, in particular, that the local representations are smooth. When I wrote it out, the formula was rather long, so I decided not to include it.That aside, here are my questions ...
1) Does this work and if so is there a cleaner solution?
2) If this works, is including the atlases for our manifolds necessary? I mean, strictly speaking, it certainly is as well as a computation that shows that the local representations are smooth. But for the purposes of this proof, I feel that including the atlases and defining the smooth local representations does little to help the presentation.

Edit:
Thinking about the problem more, I am pretty sure that h smooth follows directly from the fact that the mapping H:\mathbb{R}^{2k+2} \times \mathbb{R} \rightarrow \mathbb{R}^{2k+2} given by
<br /> H:\left(\sum_{i=1}^{2k+2}x_ie_i,t\right) \mapsto \sum_{i=1}^{k+1}\left(x_{2i-1}\cos{\pi t}-x_{2i}\sin{\pi t}\right)e_{2i-1} + \sum_{i=1}^{k+1}\left(x_{2i-1}\sin{\pi t}+x_{2i}\cos{\pi t}\right)e_{2i}<br />
is clearly smooth. If my reasoning is right here, then I think this renders the whole defining atlases thing completely unnecessary.
 
Last edited:
Physics news on Phys.org
I think you are ok. id:R^2->R^2 is homotopic to -id:R^2->R^2. You just rotate the identity by pi to get -id. And that fixes the sphere S^1. It's clearly smooth. And as you showed in an even dimensional space you can just pick the basis vectors pairwise and do the same thing.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 105 ·
4
Replies
105
Views
7K
Replies
7
Views
1K
Replies
6
Views
2K
  • · Replies 15 ·
Replies
15
Views
2K
  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 16 ·
Replies
16
Views
4K