bottlenecks to vibrational energy flow in ocs
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Observations and Phenomenology of Energy Transfer Processes Focus: Invariant Tori in the Phase Space of OCS Conclusions and Outlook Bottlenecks to vibrational energy flow in OCS Structures and mechanisms R. Pakauskas 1 C. Chandre 2 T. Uzer 3 1


  1. Observations and Phenomenology of Energy Transfer Processes Focus: Invariant Tori in the Phase Space of OCS Conclusions and Outlook Bottlenecks to vibrational energy flow in OCS Structures and mechanisms R. Paškauskas 1 C. Chandre 2 T. Uzer 3 1 Sincrotrone Trieste (ELETTRA), Trieste, Italy 2 Centre de Physique Théorique CNRS, Marseille, France 3 Georgia Institute of Technology, Atlanta GA, U.S.A. Workshop on Stability and Instability in Mechanical Systems: Applications and Numerical Tools Barcelona, 1–5 December 2008 R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  2. Observations and Phenomenology of Energy Transfer Processes Focus: Invariant Tori in the Phase Space of OCS Conclusions and Outlook Outline of the talk Observations and Phenomenology of Energy Transfer Processes 1 Transfer of Energy in Small Molecules Chaotic transport: Hydrogen in Crossed Fields Summary Focus: Invariant Tori in the Phase Space of OCS 2 Tools to Detect Resonances Unstable Tori as Transition Bottlenecks Geometry of Invariant Surfaces R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  3. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Outline of the talk Observations and Phenomenology of Energy Transfer Processes 1 Transfer of Energy in Small Molecules Chaotic transport: Hydrogen in Crossed Fields Summary Focus: Invariant Tori in the Phase Space of OCS 2 Tools to Detect Resonances Unstable Tori as Transition Bottlenecks Geometry of Invariant Surfaces R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  4. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary The OCS molecule Introduction 5 C 4.5 S R 1 R 2 O 4 ⌣ α 3.5 R 2 3 2.5 2 1.5 2 2.5 3 3.5 4 4.5 5 5.5 R 1 R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  5. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary 2.8 2.6 R 2 2.4 2.2 2 1.8 2.4 2.6 2.8 3 3.2 3.4 3.6 3.8 4 R 1 R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  6. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Obervations: Chaotic Trajectories 60 60 40 40 20 20 P 1 P 2 0 0 -20 -20 -40 -40 -60 -60 2.5 3 3.5 4 2 2.5 R 1 R 2 R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  7. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary 2.8 2.8 2.6 2.6 2.4 2.4 R 2 R 2 2.2 2.2 2 2 1.8 1.8 2.6 3 3.4 3.8 R 1 2.6 3 3.4 3.8 R 1 60 30 0 P 1 -30 -60 0 50 100 150 200 250 300 350 400 450 500 t/T 0 R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  8. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary 1 0.8 0.6 T 0 ξ P 1 0.4 0.2 60 0 30 P 1 0 -30 -60 0 100 200 300 400 500 t/T 0 R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  9. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  10. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS What are these structures allowing transitions to other parts of phase space? In three dimensions, these invariant structures can be invariant tori with dimensions one (i.e. periodic orbits), two or three. These structures can also include the stable/unstable manifolds of these objects. How are invariant structures relevant in the phenomena of capture in chaotic systems? Since Hamiltonian systems do not possess “sinks”, no such dynamical object can attract and hold forever trajectories. R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  11. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS Objects in Hamiltonian systems (such as equilibrium points, periodic orbits or invariant tori of various dimensions) according to their linear stability properties are “marginally stable” at best i.e. eigenvalues of their Jacobian matrix are unimodular. The only other qualitatively different behavior can be characterized as hyperbolic. Objects that are hyperbolic are characterized as saddle points: they both attract and repel, and typical trajectories passing by such objects are first slowed down as they approach it and then repelled as they move away from it. R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  12. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  13. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  14. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  15. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Phenomenology of OCS R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  16. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Trapping and Roaming in 3d Hamiltonians Very slow relaxation; a “numerical experiment”: 2.6 Trapping stage 2.4 Escape stage R 2 2.2 Chaos (or Roaming) 2 2.8 3 3.2 3.4 3.6 R 1 60 30 P 1 0 -30 -60 0 100 200 300 400 500 t/T 0 Look for invariant surfaces 2-tori are important R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  17. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Trapping and Roaming in 3d Hamiltonians Very slow relaxation; a “numerical experiment”: 2.6 Trapping stage 2.4 Escape stage R 2 2.2 Chaos (or Roaming) 2 2.8 3 3.2 3.4 3.6 R 1 60 30 P 1 0 -30 -60 0 100 200 300 400 500 t/T 0 Look for invariant surfaces 2-tori are important R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  18. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Trapping and Roaming in 3d Hamiltonians Very slow relaxation; a “numerical experiment”: 2.6 Trapping stage 2.4 Escape stage R 2 2.2 Chaos (or Roaming) 2 2.8 3 3.2 3.4 3.6 R 1 60 30 P 1 0 -30 -60 0 100 200 300 400 500 t/T 0 Look for invariant surfaces 2-tori are important R. Paškauskas Bottlenecks to vibrational energy flow in OCS

  19. Observations and Phenomenology of Energy Transfer Processes Transfer of Energy in Small Molecules Focus: Invariant Tori in the Phase Space of OCS Chaotic transport: Hydrogen in Crossed Fields Conclusions and Outlook Summary Trapping and Roaming in 3d Hamiltonians Very slow relaxation; a “numerical experiment”: 2.6 Trapping stage 2.4 Escape stage R 2 2.2 Chaos (or Roaming) 2 2.8 3 3.2 3.4 3.6 R 1 60 30 P 1 0 -30 -60 0 100 200 300 400 500 t/T 0 Look for invariant surfaces 2-tori are important R. Paškauskas Bottlenecks to vibrational energy flow in OCS

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