1 / 32

The Mechanism of the vdW-to-Covalent Well Transitions

The Mechanism of the vdW-to-Covalent Well Transitions. We found that a small group of trajectories ( ~10% of the sample ) make the dominant contribution to the stabilization ( ~65% of the cross section ). They describe the super-collision events:. t = 40000 a.u.

gloria-barber
Download Presentation

The Mechanism of the vdW-to-Covalent Well Transitions

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 40000 a.u.

  2. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 42000 a.u.

  3. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 44000 a.u.

  4. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 46000 a.u.

  5. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 48000 a.u.

  6. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 50000 a.u.

  7. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 51000 a.u.

  8. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 52000 a.u.

  9. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 53000 a.u.

  10. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 54000 a.u.

  11. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 55000 a.u.

  12. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 56000 a.u.

  13. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 57000 a.u.

  14. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 58000 a.u.

  15. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 60000 a.u.

  16. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 62000 a.u.

  17. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 64000 a.u.

  18. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 66000 a.u.

  19. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 68000 a.u.

  20. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 70000 a.u.

  21. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 72000 a.u.

  22. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 73000 a.u.

  23. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 74000 a.u.

  24. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 75000 a.u.

  25. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 76000 a.u.

  26. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 78000 a.u.

  27. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 80000 a.u.

  28. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 82000 a.u.

  29. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 84000 a.u.

  30. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 86000 a.u.

  31. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 88000 a.u.

  32. The Mechanism of the vdW-to-Covalent Well Transitions We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = 90000 a.u.

More Related