Prove that if $S^k$ has a non vanishing vector field, then its antipodal map is homotopy to the identity if $k$ is even.

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Prove that if $S^k$ has a non vanishing vector field, then its antipodal map is homotopy to the identity if $k$ is even.

Here is what I got so far.

Suppose we have an antipodal map $x \to -x$ of $S^k \to S^k$. For $k=1$ the antipodal just rotating the point by $180^o$. So let $R(\theta)$ be the rotation map counter clock wise by angle $\theta$, meaning

$$R(\theta)= \left( \begin{array}{ccc} Cos\theta & -sin\theta \\ sin\theta & Cos\theta \\ \end{array} \right)$$

Let $F(x,t)=R(\pi t)_x$. Know that $R$ is linear map, so it is smooth. Consider $S^k=\{x: x_1^2+x_2^2+...+x_k^2=1\}$

Now I'm stuck.

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While @Sky's answer is excellent and standard, it may be a little difficult to see the intuition behind it. Let me try to elaborate a little (warning: It's not rigorous):

Suppose that we have a non-vanishing vector field $v(x)$. Through $x$, $v(x)$, and the origin $0$, there is exactly one plane which intersects $S^n$ in a big circle. The direction of $v(x)$ uniquely (and continuously) defines a half circle (of the said big circle). Now the homotopy between $I$ and the antipodal map of $S^n$ is the exact homotopy of those of $S^1$: Move the antipodal point $-x$ along the chosen half circle towards $x$.

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If S^k has a non vanishing vector field then -I will always be homotopic to I, no matter whether k is even. Since I(x) * cos(t) + v(x) * sin(t) is the desired homopoty, where v(x) denote the normalized( that is, |v(x)|=1 ) non vanishing vector field.

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The first thing is to try to take the path $(1-t)x+t(-x)$ and project it radially on the sphere, but you cannot do it since such a path intersects the origin. But with the non vanishing vector field $v$ you can overcome that difficulty in the following way:

First, just to have a better visualization let us do the following (this is not necessary): if $\overline{v}$ is the tangent vector field (with origin at $0$), then consider $v(x)=\overline{v}(x)+x$ (now with origin at $x$).

You just walk a little bit further from $x$ in the direction of $v(x)-x$ (you can do that once $v(x)\neq0$) by the path $$\dfrac{(1-t)x+t(v(x)-x)}{|(1-t)x+t(v(x)-x)|},\quad t\in[0,1].$$ And after you reached the destiny with $t=1$ we arrived at the point $v(x)/|v(x)|$, and now the path $(1-s)v(x)/|v(x)|+s(-x)$ never intersects the origin since $\overline{v}(x)$ is orthogonal to $-x$. Therefore you project it radially on the sphere and glue this path with the previous one, so you get the homotopy

$$H(x,t)=\begin{cases} \dfrac{(1-2t)x+2t(v(x)-x)}{|(1-2t)x+2t(v(x)-x)|}\quad\text{if}\quad t\in[0,1/2]\\ \dfrac{(2-2t)v(x)+(2t-1)(-x)}{|(2-2t)v(x)+(2t-1)(-x)|}\quad\text{if}\quad t\in[1/2,1], \end{cases}$$ which is clearly a homotopy between the identity and the antipodal map.