210 likes | 325 Views
Spectroscopic signatures of a saddle point. Modelled on HCP as a perturbed spherical pendulum. Spherical pendulum. P. C. θ. H. Outline. Model Hamiltonian Properties of spherical pendulum states Classical trajectories of the coupled model Anharmonic resonances Polyad structure
E N D
Spectroscopic signatures of a saddle point Modelled on HCP as a perturbed spherical pendulum
Spherical pendulum P C θ H
Outline • Model Hamiltonian Properties of spherical pendulum states Classical trajectories of the coupled model Anharmonic resonances Polyad structure • Rotation/vibrational dynamics of HCP bending states Extended RKR potential function Anomalous magnitudes of vibn/rotn parameters • Summary
Quantum pendulum states 2.0 1.0 E/V0 Diagonalize in a spherical harmonic basis 0.0 -1.0 k
Semiclassical pendulum states Complete analytical solution in terms of Elliptic integrals, which yields the following limiting formulae for k=0
Polyad structure E<B Inside Fermi res Outside Measured from lowest level of polyad Mean polyad number np=2vs+vb
Polyad structure 0<E<2B Vibrating states Rotating states
Importance of resonance terms ΔE np E
HCP bend monodromy plot
Summary • Classical and semiclassical methods used to illuminate dynamics of HCP-like model • Classical bending frequency function and Heisenberg matrix elements used to model occurrence and strength of 1:n resonances • RKR plus ab initio information used to determine realistic HCP bending potential • Anomalously large vibn/rotn interaction parameters explained and predicted
Acknowledgements • M P Jacobson (UCSF) • C D Cooper (Oxford) • UK EPSRC References • M P Jacobson and M S Child JCP 114, 250 (2001) • M P Jacobson and M S Child JCP 114, 262 (2001) • M P Jacobson and M S Child JPC 105, 2834 (2001) • M S Child, M P Jacobson and C D Cooper JPC 105, 10791 (2001)