Define the map P:TSn→SnbyP((x,v))=x+v∥x+v∥
where
TSn={(x,v)∈Sn ×Rn+1∣v⊥x}
This map is used in the book of Alain Hatcher, Algebraic topology, to give a proof for the fact that every vector field on even spheres must vanish at some point of the sphere.
Question:
Does P define a (nontrivial) fiber bundle?
Define the Hamiltonian function H:TSn→R with H(x,v)=∥P(x,v)−x∥2 where the latter norm is the standard Euclidean norm on Rn+1. What can be said about the dynamical behavior of the corresponding Hamiltonian vector field XH? Are there any periodic orbit?
- Assume that V is a vector field on the sphere. To V, we associate a self map f(x)=P(x,V(x)) on the sphere. Are there some relations between the continuous dynamics of V and the discrete dynamics of f. Note that V and f have the same fixed points.
This post imported from StackExchange MathOverflow at 2016-11-05 15:54 (UTC), posted by SE-user Ali Taghavi