1. Rovibronic Energy Topography I: Tensor Eignvalue Structure and Tunneling Effects in Low-Symmetry Species-Clusters of High Symmetry Molecules Justin Mitchell, William Harter University of Arkansas Fayetteville, AR 72701 Please Load.pdf version

2. Understanding Eigensolutions We want to interpret physically numerical solutions and begin to understand dynamics.

3. How to get more information 1. Write Hamiltonian in Tensor Expansion 2. Phase Space Plots of Tensors 3. Topography of Level Clustering (fine structure) 4. Symmetry Analysis of Cluster Splitting (super-fine structure)

4. How to get more information 1. Write Hamiltonian in Tensor Expansion 2. Phase Space Plots of Tensors 3. Topography of Level Clustering (fine structure) 4. Symmetry Analysis of Cluster Splitting (super-fine structure)

5. Clustering in Rotational Sub-Levels Level Clusters Appear in Diagonalization of 4th, 6th, 8th Rank Rotational Hamiltonian. Spontaneous Symmetry Breaking of Octahedral O h to Cyclic C 4, C 3, C 2 and C 1. Rotational Energy Surface display 4th, 6th and 8th rank tensors combinations.

6. How to get more information 1. Write Hamiltonian in Tensor Expansion 2. Phase Space Plots of Tensors 3. Topography of Level Clustering (fine structure) 4. Symmetry Analysis of Cluster Splitting (super-fine structure)

7. Rotational Energy Surface Phase Space Plot. Constant Total Angular Momentum, J. Angular momentum follows constant energy contours in molecular frame. Contours are Eigenvalues J=30

8. Level Clustering Fewer Levels Than Expected. Level clusters may contain 6, 8, 12, 24 or 48 rotational levels. Phase Space Pockets have Local Symmetry C 4, C 3, C 2, C v or C 1. Resonance or tunneling occurs between the equivalent phase space regions. This slightly splits the Clusters. J=30

9. How to get more information 1. Write Hamiltonian in Tensor Expansion 2. Phase Space Plots of Tensors 3. Topography of Level Clustering (fine structure) 4. Symmetry Analysis of Cluster Splitting (super-fine structure)

10. J=30 T [4] All T [4] - C 3 and C 4 Clusters

11. J=30 T [4] All T [4] - C 3 and C 4 Clusters C.W. Patterson, R.S. McDowell, N.G. Nereson, B.J. Krohn, J.S.Wells, and F.R.Peterson, J. Mol. Spec. 91, 416 (1982)

12. No C 3, Start C 2 Clusters

13. Even T [4], T [6]

14. C 4 Equal C 3 Clusters

15. All T [6]

16. No C 2, C 4 Clusters

17. All T [4] - C 3 and C 4 Clusters

18. Include T [4], T [6], T [8]

19. Big level cluster! 24 Equivalent valleys 24-level cluster

20. How to get more information 1. Write Hamiltonian in Tensor Expansion 2. Phase Space Plots of Tensors 3. Topography of Level Clustering (fine structure) 4. Symmetry Analysis of Cluster Splitting (super-fine structure)

21. Analyze Splitting Start With Octahedral Hamiltonian. Write All Tunnelings Between Equivalent Local Symmetry Regions. Use This Hamiltonian with Known Eigenvectors. J=30 Tunneling “paths”

22. Analyze Splitting J=30

23. Analyze Splitting

24. Next Talk Similar Splittings, More Sophisticated Method Keep Track of Tunneling Paths with Group Parameters Method To Find What Tunneling Paths Spoil the Local Symmetry

25. Rovibronic Energy Topography I: Tensor Eignvalue Structure and Tunneling Effects in Low-Symmetry Species-Clusters of High Symmetry Molecules Justin Mitchell, William Harter University of Arkansas Fayetteville, AR 72701