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  • 1
    Book
    Book
    New York, NY :Springer,
    Title: Quantum dynamics with trajectories /; 28
    Author: Wyatt, Robert Eugene
    Publisher: New York, NY :Springer,
    Year of publication: 2005
    Pages: XXI, 405 S. : , Ill., graph. Darst.
    Series Statement: Interdisciplinary applied mathematics 28
    ISBN: 0-387-22964-7 , 978-0-387-22964-5
    Type of Medium: Book
    Language: English
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 10794-10805 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present an investigation of Hermite polynomials as a basic paradigm for quantum dynamics, and make a thorough comparison with the well-known Chebyshev method. The motivation of the present study is to develop a compact and numerically efficient formulation of the spectral filter problem. In particular, we expand the time evolution operator in a Hermite series and obtain thereby an exponentially convergent propagation scheme. The basic features of the present formulation vìs a vìs Chebyshev scheme are as follows: (i) Contrary to the Chebyshev scheme Hamiltonian renormalization is not needed. However, an arbitrary time scaling may be necessary in order to avoid numerical hazards, and this time scaling also provides a leverage to accelerate the convergence of the Hermite series. We emphasize the final result is independent of the arbitrary scaling. (ii) As with the Chebyshev scheme the method is of high accuracy but not unitary by definition, and thus any deviation from unitarity may be used as a guideline for accuracy. The calculation of expansion coefficients in the present scheme is extremely simple. To contrast the convergence property of present method with that of the Chebyshev one for finite time propagation, we have introduced a time–energy scaling concept, and this has given rise to a unified picture of the overall convergence behavior. To test the efficacy of the present method, we have computed the transmission probability for a one-dimensional symmetric Eckart barrier, as a function of energy, and shown that the present method, by suitable time–energy scaling, can be very efficient for numerical simulation. Time–energy scaling analysis also suggests that it may be possible to achieve a faster convergence with the Hermite based method for finite time propagation, by a proper choice of scaling parameter. We have further extended the present formulation directed toward the spectral filter problem. In particular, we have utilized the Gaussian damping function for the purpose. The Hermite propagation scheme has allowed all the time integrals to be done fully analytically, a feature not completely shared by the Chebyshev based scheme. As a result, we have obtained a very compact and numerically efficient scheme for the spectral filters to compute the interior eigenspectra of a large rank eigensystem. The present formulation also allows us to obtain a closed form expression to estimate the error of the energies and spectral intensities. As a test, we have utilized the present spectral filter method to compute the highly excited vibrational states for the two-dimensional LiCN (J=0) system and compared with the exact diagonalization result. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 3326-3334 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We report the results of a detailed quantum dynamical investigation of energy flow in 30-mode benzene. The CH(ν=2) overtone was examined by propagating an initial bright state in an active space of dimension N=16000 for 9.6 ps. Two sets of initial conditions were investigated: one in which the overtone energy was distributed as in one of the E1u symmetries appropriate for dipole excitation from the ground state and the other in which the overtone energy was localized in a single CH stretching motion. The rate and extent of energy flow out of the CH chromophore is dictated by the choice of initial conditions. Conclusions from the model where energy is localized in a single CH stretch indicate that the meta in-plane CH wags and para out-of-plane CH bend are the major recipients of bursts of energy for t≤300 fs; the ipso CH stretch retains only 10% of the overtone energy by 9.6 ps. For the E1u model, the initially excited CH stretches retain 30% of the overtone energy in long time; the ipso out-of-plane CH bend is activated before the ipso in-plane CH wag and with less energy, mimicing the results of previous classical investigations. For both models examined, energy is equipartitioned within the CC stretches, in-plane CH wags, and out-of-plane CH bends by 9.6 ps; the magnitude of energy taken up by the CC stretches and in-plane CH wags is the same. CCC in-plane bends and CCCC out-of-plane ring torsions are of relatively minor importance (on the time scale considered) in intramolecular vibrational energy redistribution in benzene. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 109 (1998), S. 10732-10739 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The results of large-scale quantum mechanical calculations of the CH(v=2) 1st overtone spectrum for 30-mode benzene are reported. This overtone was chosen for investigation because of its high degree of fragmentation and resulting complexity compared to spectra for the fundamental and higher overtones. These calculations use the best available ab initio force field supplemented by higher-order terms for the CH stretch–wag interaction. The dynamical calculations were conducted in large active spaces with 12 000 or 16 000 vibrational basis functions. The recursive residue generation method was used to compute residues (intensities) and eigenvalues. From these quantities, the lineshape function, survival probabilities, and vibrograms were computed. Wherever possible, these results were compared to experimental overtone spectra and to other computational results. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 7047-7054 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We continue a study in which we statistically analyze the dynamics of vibrational energy flow in a model system of anharmonic oscillators which are nonlinearly coupled, with a local topology. Average spectra are obtained from individual spectra of many basis states of similar energy, for different values of the magnitude of the coupling between states. The survival probabilities of the density are then determined from the average spectra. When the average fluctuation in spectral intensities is small then the density survival probability closely follows the average survival probability presented in our earlier paper for short times. For longer times, when the average survival probability shows a power law decay, this decay does not appear in the density survival probability. In addition, when spectral fluctuations are large, the two survival probabilities differ strongly. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 3580-3591 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A hybrid quantum/classical approach for treating the vibrational and translational motion of the I2 molecule inside a cold Ar matrix is implemented in the control of vibrational wave packet localization on the excited (A) electronic surface of I2. Quantum control was performed in the weak-field regime at six different temperatures to examine thermal effects on the dynamics of I2 inside the lattice and on the degree of control that can be achieved for this system. It was found in this study that an increase in temperature from 0 to 75 K leads to a moderate decrease in the degree of control achieved. The role played by I2 rotation on control was also shown to be minimal under the conditions examined in this work. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 10730-10737 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The quantum trajectory method (QTM) was recently developed to solve the hydrodynamic equations of motion in the Lagrangian, moving-with-the-fluid, picture. In this approach, trajectories are integrated for N fluid elements (particles) moving under the influence of both the force from the potential surface and from the quantum potential. In this study, distributed approximating functionals (DAFs) are used on a uniform grid to compute the necessary derivatives in the equations of motion. Transformations between the physical grid where the particle coordinates are defined and the uniform grid are handled through a Jacobian, which is also computed using DAFs. A difficult problem associated with computing derivatives on finite grids is the edge problem. This is handled effectively by using DAFs within a least squares approach to extrapolate from the known function region into the neighboring regions. The QTM–DAF is then applied to wave packet transmission through a one-dimensional Eckart potential. Emphasis is placed upon computation of the transmitted density and wave function. A problem that develops when part of the wave packet reflects back into the reactant region is avoided in this study by introducing a potential ramp to sweep the reflected particles away from the barrier region. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 109 (1998), S. 8330-8337 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Computational studies based upon ensembles of quasiclassical trajectories are presented for 21-mode (planar) benzene, with which we examined relaxation of the first and second (v=2,3) CH stretch overtones. The most complete ab initio force field available for this molecule was used for short time (t〈240 fs) and long time (t=2.4 ps) dynamical calculations. Local mode analyses indicate that energy flow from the initially excited CH stretch is fast (t〈240 fs) and irreversible. For both overtones examined, energy from the CH chromophore activates the following local modes in sequence: ipso in-plane CH wag, adjacent CC stretch, terminal CC stretch, ortho CH in-plane wag, meta CH in-plane wag, intermediate CC stretch, meta CH stretch, para CH in-plane wag, and para CH stretch. Long time calculations indicate that the in-plane CH wag and CH stretching local modes are at steady-state quantities by 2.4 ps, while the CC stretches and CCC bends continue to take on energy. The ortho and meta CH stretches were of minor importance in intramolecular vibrational energy redistribution in benzene, gaining little or no energy over the time scales we studied. Survival probabilities indicate that the half life of the excited CH stretch decreases by almost two thirds as the overtone energy is raised. The results of our study are compared to other classical and quantum dynamical investigations of benzene and are found to be in good qualitative agreement. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 9483-9496 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In this series, the multiple time scales and mechanisms of intramolecular vibrational-energy redistribution (IVR) present in the CH overtones of fluoroform is investigated. In part II, we analyze the ab initio vibrational spectrum and dynamics of the vCH=1 and vCH=2 regions, explicitly treating all vibrational degrees of freedom. A wave operator sorting algorithm is used to develop an efficient vibrational basis. Spectral transformation, by a filtered-Lanczos method, is used to accelerate eigenstate analysis. The theoretical spectrum of the fundamental is nontrivial, predicting a close triplet of lines (width 〈6 cm−1) centered at 3048.3 cm−1 and a weak line 20 cm−1 upfield, due to coupling with a small subsystem of background modes: ν4±+ν5±+ν6±, ν2+ν4±+ν6±, and ν3+2ν5. Furthermore, these background states mix with one another and other nearby background states via resonances ω5(approximate)(ω3+ω6), ω2(approximate)ω5, and (ω4+ω6)(approximate)(ω3+ω5). An effective Hamiltonian is used to assess chromophore–background and background–background coupling. In contrast, the first overtone exhibits no strong background resonances, rather the background modes function as a weakly coupled reservoir. IVR time scales and eigenstate convergence, with respect to the active space, are presented. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 4406-4413 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The quantum trajectory method (QTM) for time-dependent wave packet dynamics involves integration of the de Broglie–Bohm hydrodynamic equations for the evolving probability fluid [C. Lopreore and R. E. Wyatt, Phys. Rev. Lett. 82, 5190 (1999)]. The equations of motion for discretized elements of the probability fluid (particles) are integrated in the Lagrangian, moving with the fluid, picture. These fluid elements move under the influence of both the usual potential energy function and the quantum potential, which involves the curvature of the quantum amplitude. The quantum potential and the quantum force are evaluated using a moving weighted least squares algorithm. As a demonstration of applicability, the QTM is applied to a model collinear reaction with an activation barrier. The reaction probabilities are in good agreement with exact quantum results, even for a relatively small number of particles in the ensemble. The QTM accurately describes tunneling using only real valued trajectories. In addition to the reaction probability, plots are presented to show the probability density and the flux distributions at several time steps during the reaction. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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