• Aucun résultat trouvé

2 Annular billiard dynamics in a strong laser field

N/A
N/A
Protected

Academic year: 2022

Partager "2 Annular billiard dynamics in a strong laser field"

Copied!
1
0
0

Texte intégral

(1)

Annular billiard dynamics in a strong laser field

A. Kamor1,2, F. Mauger1,2, C. Chandre2, & T. Uzer1

1 School of Physics, Georgia Institute of Technology, Atlanta, GA 30332-0430, USA

2 Centre de Physique Th´eorique, CNRS – Aix-Marseille Universit´e, Campus de Luminy, case 907, 13288 Marseille cedex 09, France

[email protected]

We analyze the dynamics of a valence electron of the buckminsterfullerene molecule (C60) subjected to a circularly polarized laser field by modeling it with the motion of a classical particle in an annular billiard. We show that the phase space of the billiard model gives rise to three distinct trajectories :

“Whispering gallery orbits”, which only hit the outer billiard wall, “daisy orbits” which hit both billiard walls (while rotating solely clockwise or counterclockwise for all time), and orbits which only visit the downfield part of the billiard, as measured relative to the laser term. These trajectories, in general, maintain their distinct features, even as intensity is increased from 1010 to 1014 W·cm−2. We attribute this robust separation of phase space to the existence of twistless tori.

To perform this analysis of an atomic system we use many tools from nonlinear dynamics applied to the Hamiltonian framework within which we work. These tools are Poincar´e sections to observe the dynamics, a frequency analysis to identify non-KAM tori, i.e. twistless tori, and an identification of periodic orbits to better understand the dynamics.

R´ ef´ erences

1. A. Kamor, F. Mauger, C. Chandre, and T. Uzer - Annular billiard dynamics in a circularly polarized strong laser field - Physical Review E - 85, 016204 (2012)

Références

Documents relatifs

A strategy of the proof of the Tree Conjecture is the following: the symbolic dynamics of any periodic trajectory is defined by a sequence of flowers (unions of singular leaves) in

In Section 4 we recall different facts about word combinatorics, billiard maps and the relationship between the billiard map and rotations on the torus.. In section 5 we prove

We give sufficient and necessary conditions for a periodic orbit to be λ-stable and prove that the set of d-gons having at most finite number of λ-stable periodic orbits is dense is

We deduce the existence of an open set of tetrahedra which have a periodic orbit of length four (generaliza- tion of Fagnano’s orbit for triangles), moreover we can study completly

Le cinquième et dernier chapitre est consacré à des applications numériques divers sont établis pour vérifier l'exactitude de la nouvelle théorie du premier

Then we will use the following proposition, which follows from the fact that the reflection law with respect to a non-isotropic line permutes two isotropic lines, [14], corollary

what is a triangular complex orbit in Subsection 2.3; then, in Section 3 we introduce the definition and we study properties of complex circumscribed circles to such orbits:

This means that even if the source is a point excitation with strong directivity (like the torque considered in the examples), the resulting vibrational field will be diffuse in