- Commit
- 523f51458818b70b8c697dbd77f0c00e998ed289
- Parent
- d14391d0b7b088662466bc5b41a6563b6459d4bd
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Fixed some typos
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 some typos
2 files changed, 3 insertions, 3 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/applications.tex | 4 | 2 | 2 |
Modified | sections/introduction.tex | 2 | 1 | 1 |
diff --git a/sections/applications.tex b/sections/applications.tex @@ -510,7 +510,7 @@ however, is the following consequence of Morse's theorem. as \(X \to 0\). Let \(\gamma\) be as in \textbf{(i)}. Since \(\gamma\) has no conjugate - points, it follows from Morses's index theorem that \(T_\gamma^- \Omega_{p q} + points, it follows from Morse's index theorem that \(T_\gamma^- \Omega_{p q} M = 0\). Furthermore, by noticing that any piece-wise smooth \(X \in \ker A_\gamma\) is Jacobi field vanishing at \(p\) and \(q\) one can also show \(T_\gamma^0 \Omega_{p q} M = 0\). Hence \(T_\gamma \Omega_{p q} M = @@ -553,7 +553,7 @@ classical formulation: we can find curves \(\eta = i(v)\) shorter than This concludes our discussion of the applications of our theory to the geodesics problem. We hope that this short notes could provide the reader with -a glimpse of the rich theory of the calculus of variations and global anylisis +a glimpse of the rich theory of the calculus of variations and global analysis at large. We once again refer the reader to \cite[ch.~2]{klingenberg}, \cite[ch.~11]{palais} and \cite[sec.~6]{eells} for further insight on modern variational methods.
diff --git a/sections/introduction.tex b/sections/introduction.tex @@ -75,7 +75,7 @@ discuss neither technicalities nor more involved applications of the theory we will develop. In particular, we leave the intricacies of Palais' discussion of condition (C) --- wich can be seen as a substitute for the failure of a proper Hilbert space +-- which can be seen as a substitute for the failure of a proper Hilbert space to be locally compact \cite[ch.~2]{klingenberg} -- and its applications to the study of closed geodesics out of this notes. As previously stated, many results are left unproved, but we will include references to other materials containing