The Liouville-Arnold theorem describes the topological structure of completely integrable Hamiltonian systems and provides the existence of action-angle coordinates, in which the Hamiltonian motion is affine-linear. I will show examples of completely integrable systems and classical approaches to solve these explicitly via the construction of action-angle coordinates and quadrature.
Termin
Dienstag, 14.01.2025
| 09.15 bis 11.00 Uhr
|
M-Nachrichten
Seminar "Poisson geometry and integrable systems": Christian Offen: Solving completely integrable systems by quadrature (II)
Ort: E 2.304