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Spectroscopic signatures of a saddle point
Modelled on HCP as a perturbed spherical pendulum
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Spherical pendulum P C θ H
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Outline Properties of spherical pendulum states Model Hamiltonian
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
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Model Hamiltonian
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Quantum pendulum states
2.0 1.0 E/V0 Diagonalize in a spherical harmonic basis 0.0 -1.0 k
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Semiclassical pendulum states
Complete analytical solution in terms of Elliptic integrals, which yields the following limiting formulae for k=0
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Surfaces of section and periodic orbits
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Periodic orbit bifurcations
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Periodic orbit frequencies
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Polyad structure E<B
Inside Fermi res Outside Measured from lowest level of polyad Mean polyad number np=2vs+vb
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Polyad structure 0<E<2B
Vibrating states Rotating states
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Importance of resonance terms
np E
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HCP extended RKR bending potential
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HCP bend monodromy plot
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l doubling
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Vibration rotation constants
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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
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Acknowledgements References 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, (2001)
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