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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 6378-6390 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Nondegenerate Rayleigh–Schrödinger perturbation theory diverges when applied to nearly resonant molecular vibrations. Traditionally, this divergence has been avoided by using quasidegenerate perturbation methods, such as partitioning, or Van Vleck's transformation approach. In this paper, we present a method of resummation, called reconstruction, that is appropriate for nearly degenerate systems displaying a strong mixing between a finite number of zeroth order states. In order to implement the approach, a set of strongly interacting states must be identified. The method then produces a pseudoconvergent power series expansion for an effective secular equation from the divergent perturbation expansion of the energies of the strongly interacting states. The effective secular equation has a low polynomial degree, and may readily be solved numerically to yield resummed values of the energies. We compare reconstruction to diagonal Padé approximation, and find that Padé approximants resum energies in the vicinity of avoided crossings poorly, yielding levels that cross where the actual eigenvalues repel. Reconstruction, however, correctly reproduces the avoided crossing behavior.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 86 (1987), S. 279-307 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The Fourier transform approach to EBK quantization, previously applied to nonresonant systems with up to four degrees of freedom [J. Chem. Phys. 83, 2990 (1985)], is extended to the case of strongly resonant classical motion. The classical mechanics of systems with 3:4, 1:2, and 1:1 resonances is examined in detail from the Fourier transform point of view, and the results of nonlinear resonance analysis used to interpret numerical trajectory Fourier spectra. Calculation of classical actions and numerical construction of the angle parametrization of invariant tori is described, and the relation between spectral frequency assignments and the choice of good action-angle variables investigated. It is shown that correct quantization conditions for arbitrary resonant motion can be determined by direct numerical evaluation of Maslov indices. Semiclassical eigenvalues are reported for the 3:4, 1:2, and 1:1 resonant systems.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 87 (1987), S. 284-302 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: This paper addresses the general problem of zeroth order representation of resonant dynamics. We investigate the classical, quantum mechanical, and semiclassical transformation properties of two-dimensional isotropic and anisotropic uncoupled harmonic oscillators. The classical and quantal theories are presented in a manner that emphasizes the strong correspondence between the two, and in particular, the SU(2) symmetry exhibited by both the classical and quantum oscillators. The classical canonical transformations relating the action-angle variables appropriate for normal, local, and precessional motion of the isotropic oscillator are derived by explicit calculation of the generating functions. By employing a simple mapping relating the anisotropic and isotropic oscillators, expressions for action-angle variables appropriate for the topology of an arbitrary m:n resonance are determined. The resulting invariant tori are compared with the corresponding quantum mechanical wave functions and phase space densities. The relationship between the classical and quantum mechanical theories is illustrated by determining semiclassical approximations to the unitary transformation matrix elements, which are given in terms of the classical generating functions. Applications to problems of current interest, such as the adiabatic switching method for semiclassical quantization of nonseparable systems, are briefly discussed.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 86 (1987), S. 6270-6282 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The method of algebraic quantization, a semiclassical analog of Van Vleck perturbation theory, is applied to multidimensional resonant, nonresonant, and nearly resonant systems. perturb, a special purpose program written in C, is utilized to implement classical perturbation theory efficiently to high order. States corresponding to both regular and chaotic classical regimes are quantized, and accurate eigenvalues obtained in both cases. Various quantization rules are compared, and a novel symmetry preserving rule is given which leads to good agreement with quantum mechanics. The method is able to reproduce purely quantum mechanical splittings to very good accuracy. Algebraic quantization combined with Padé resummation is used to determine energy eigenvalues for a resonant system with five degrees of freedom.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 83 (1985), S. 5369-5379 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A simple theoretical model is developed for relative band intensities in multiresonant molecular three-photon ionization. A specific case is considered in which a dissociative system of states exists at the energy of the first photon and a discreet level system at the second. A third photon ionizes the molecule. Experimentally such a system shows non-Franck–Condon transitions with relative intensities that depend on laser power. Model calculations trace this dependence to the coherent preparation of a superposition state over the levels at the energy of the first photon that lie within the power-broadened bandwidth of the laser. For reasonable choice of field and molecule parameters, the model reproduces well the power-dependent band intensities reported in the previous paper for NO2.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 2089-2098 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We semiclassically quantize a classical analog Hamiltonian, derived using the classical electron formalism of Meyer and Miller, for the linear approximation to the Jahn–Teller E×e system. Quantization is achieved for realistic values of the nonadiabatic coupling parameter, by means of the method of adiabatic switching. The results are found to be in reasonable agreement with quantum mechanical eigenvalues, and a useful qualitative picture of the associated nonadiabatic dynamics is obtained.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 2648-2668 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A four-dimensional symplectic (Hamiltonian) mapping of the type studied by Gaspard and Rice is used to model the predissociation of the van der Waals complex He–I2. Phase space structure and unimolecular decay in this mapping are analyzed in terms of a general approach recently developed by Wiggins. The two-dimensional area preserving map obtained by restricting the 4D map to the T-shaped subspace is studied first. Both the Davis–Gray theory and the analog of the alternative RRKM theory of Gray, Rice, and Davis for discrete maps are applied to estimate short-time decay rates. A four-state Markov model involving three intramolecular bottlenecks (cantori) is found to give a very accurate description of decay in the 2D map at short to medium times. The simplest version of the statistical Davis–Gray theory, in which only a single intermolecular dividing surface is considered, is then generalized to calculate the fragmentation rate in the full 4D map as the ratio of the volume of a four-dimensional turnstile lobe and a four-dimensional complex region enclosed by a multidimensional separatrix. Good agreement with exact numerical results is found at short times. The alternative RRKM theory is also applied, and is found to give a level of agreement with the Davis–Gray theory comparable to the 2D case. When the height of the barrier to internal rotation in the van der Waals potential is increased, however, it is found that volume-enclosing turnstile no longer exist in the 4D phase space, due to the occurrence of homoclinic tangency. The implications of this finding for transport theories in multimode systems are briefly discussed.
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  • 8
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 91 (1987), S. 3721-3730 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 93 (1989), S. 3877-3880 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 156-179 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In this paper we study the classical and quantum mechanics of the 3-mode Baggot vibrational Hamiltonian for H2O. Our aim is to classify and assign highly-excited quantum states based upon a knowledge of the classical phase space structure. In particular, we employ a classical template formed by the primary resonance channels in action space, as determined by Chirikov resonance analysis. More detailed analysis determining the exact periodic orbits and their bifurcations and families of resonant 2-tori for the Baggot Hamiltonian confirms the essential correctness of the Chirikov picture. It is emphasized that the primary periodic orbits alone do not define a suitable phase space skeleton; it is important to consider higher dimensional invariant structures, such as 2-tori and 3-tori. Examining the manifold of quantum states for a given superpolyad number P=n1+n2+nb/2 reveals sequences of eigenstates that progress along the classical resonance zones. These sequences provide insight into the nature of strongly mixed states found in the vicinity of the resonance junction. To further explore the classical-quantum correspondence, we have also computed eigenstate Husimi phase space distribution functions and inverse participation ratios. It is thereby possible to provide dynamically based assignments for many states in the manifold of states with superpolyad number P=16. © 1997 American Institute of Physics.
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