- Commit
- f09d3c968ceb744a4f9c68e28289da9c4269f747
- Parent
- 66b9c09f3dcc2b2c30975bc97f4f49ceaddfb61a
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Fixed a small typo
Riemannian Geometry course project on the manifold H¹(I, M) of class H¹ curves on a Riemannian manifold M and its applications to the geodesics problem
Fixed a small typo
1 file changed, 9 insertions, 9 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/structure.tex | 18 | 9 | 9 |
diff --git a/sections/structure.tex b/sections/structure.tex @@ -441,15 +441,15 @@ extended to a canonical isomorphism of vector bundles, as seen in\dots \end{proof} At this point it may be tempting to think that we could now define the metric -of \(H^1(I, M)\) in a fiber-wise basis via the identification \(T_\gamma -H^1(\gamma^* TM) \cong H^1(\gamma^* TM)\). In a very real sense this is what we -are about to do, but unfortunately there are still technicalities in our way. -The issue we face is that proposition~\ref{thm:h0-bundle-is-complete} only -applies for \emph{smooth} vector bundles \(E \to I\), which may not be the case -for \(E = \gamma^* TM\) if \(\gamma \in H^1(I, M)\) lies outside of -\({C'}^\infty(I, M)\). In fact, neither \(\langle X , Y \rangle_0\) nor -\(\langle \, , \rangle_1\) are defined \emph{a priori} for \(X, Y \in -H^0(\gamma^* TM)\) with \(\gamma \notin {C'}^\infty(I, M)\). +of \(H^1(I, M)\) in a fiber-wise basis via the identification \(T_\gamma H^1(I, +M) \cong H^1(\gamma^* TM)\). In a very real sense this is what we are about to +do, but unfortunately there are still technicalities in our way. The issue we +face is that proposition~\ref{thm:h0-bundle-is-complete} only applies for +\emph{smooth} vector bundles \(E \to I\), which may not be the case for \(E = +\gamma^* TM\) if \(\gamma \in H^1(I, M)\) lies outside of \({C'}^\infty(I, +M)\). In fact, neither \(\langle X , Y \rangle_0\) nor \(\langle \, , +\rangle_1\) are defined \emph{a priori} for \(X, Y \in H^0(\gamma^* TM)\) with +\(\gamma \notin {C'}^\infty(I, M)\). Nevertheless, we can get around this limitation by extending the metric \(\langle \, , \rangle_0\) and the covariant derivative \(\frac\nabla\dt =