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Titlebook: Classical and Quantum Dynamics; From Classical Paths Walter Dittrich,Martin Reuter Textbook 20175th edition Springer International Publishi

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31#
發(fā)表于 2025-3-26 23:25:08 | 只看該作者
Jacobi Fields, Conjugate Points,particular, we want to investigate the conditions under which a path is a minimum of the action and those under which it is merely an extremum. For illustrative purposes we consider a particle in two-dimensional real space.
32#
發(fā)表于 2025-3-27 02:33:38 | 只看該作者
Action-Angle Variables,..) is the generator of a canonical transformation to new constant momenta .. (all .. are ignorable), and the new Hamiltonian depends only on the ..: . = . = .(..). Besides, the following canonical equations are valid:
33#
發(fā)表于 2025-3-27 08:38:42 | 只看該作者
Time-Independent Canonical Perturbation Theory, conservative, .∕. = 0,?and periodic in both the unperturbed and perturbed case. In addition to periodicity, we shall require the Hamilton–Jacobi equation to be separable for the unperturbed situation. The unperturbed problem ..(..) which is described by the action-angle variables .. and .. will be assumed to be solved.
34#
發(fā)表于 2025-3-27 10:27:45 | 只看該作者
Removal of Resonances,rs appear in the expression for the adiabatic invariants. We now wish to begin to locally remove such resonances by trying, with the help of a canonical transformation, to go to a coordinate system which rotates with the resonant frequency.
35#
發(fā)表于 2025-3-27 17:30:51 | 只看該作者
36#
發(fā)表于 2025-3-27 20:17:02 | 只看該作者
The KAM Theorem,..., ..) converges (according to Newton’s procedure) and thus the invariant tori are not destroyed. The KAM theorem is valid for systems with two and more degrees of freedom. However, in the following, we shall deal exclusively with the case of two degrees of freedom.
37#
發(fā)表于 2025-3-27 22:01:20 | 只看該作者
38#
發(fā)表于 2025-3-28 05:14:16 | 只看該作者
39#
發(fā)表于 2025-3-28 07:36:54 | 只看該作者
40#
發(fā)表于 2025-3-28 11:41:20 | 只看該作者
Reluctant Reinforcement Learning..) is the generator of a canonical transformation to new constant momenta .. (all .. are ignorable), and the new Hamiltonian depends only on the ..: . = . = .(..). Besides, the following canonical equations are valid:
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