- Commit
- 168e4f08b46c79458a63cd8900e32ab9282f8144
- Parent
- e650504db371aa9e0dce48f8c65ee01b4ce47fc9
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Added a conclusion to the last section
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
Added a conclusion to the last section
1 file changed, 15 insertions, 12 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/applications.tex | 27 | 15 | 12 |
diff --git a/sections/applications.tex b/sections/applications.tex @@ -542,15 +542,18 @@ We should point out that part \textbf{(i)} of theorem~\ref{thm:jacobi-darboux} is weaker than the classical formulation of the Jacobi-Darboux theorem -- such as in theorem 5.5.3 of \cite{gorodski} for example -- in two aspects. First, we do not compare the length of curves \(\gamma\) and \(\eta \in U\). This could -be amended by showing that the length functional \(L : H^1(I, M) \to \RR\) -is smooth and that its Hessian \(d^2 L_\gamma\) is given by \(C \cdot d^2 -E_\gamma\) for some \(C > 0\). - -Secondly, unlike the classical formulation we only consider curves in an -\(H^1\)-neighborhood of \(\gamma\) -- instead of a neighborhood of \(\gamma\) -in \(\Omega_{p q} M\) in the uniform topology. On the other hand, part -\textbf{(ii)} is definitively an improvement of the classical formulation: we -can find curves \(\eta = i(v)\) shorter than \(\gamma\) already in an -\(H^1\)-neighborhood of \(\gamma\). - -We hope that short notes could provide the reader +be amended by showing that the length functional \(L : H^1(I, M) \to \RR\) is +smooth and that its Hessian \(d^2 L_\gamma\) is given by \(C \cdot d^2 +E_\gamma\) for some \(C > 0\). Secondly, unlike the classical formulation we +only consider curves in an \(H^1\)-neighborhood of \(\gamma\) -- instead of a +neighborhood of \(\gamma\) in \(\Omega_{p q} M\) in the uniform topology. On +the other hand, part \textbf{(ii)} is definitively an improvement of the +classical formulation: we can find curves \(\eta = i(v)\) shorter than +\(\gamma\) already in an \(H^1\)-neighborhood of \(\gamma\). + +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 +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.