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c) coefficients, which are chosen to coincide with the calculations (for details, see ref 6).
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85034288971
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To simulate energy exchange between the dynamical collective shape variables and the other degrees of freedom of the cluster, one can include frictional terms in the equations of motion. This would result in damping of the collective shape dynamics; for the short trajectories used here, such effects are not expected to have a significant influence.
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24
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85034276029
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-6 eV.
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26
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0000017029
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v(a,b) by solving the nonlinear Bohr-Mottelson Hamiltonian (see: Kumar, K.; Baranger, M. Nucl. Phys. A 1967, 92, 608). Work along this line for the NeNePo of the silver trimer is in progress.
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Plenum: New York, Figure 3.56
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The experiments in ref 13 used photons of 3.1 eV for electron detachment and (double) photons of 5.9-6.36 eV for ionization, while the plasmon energy in small silver clusters is about 4.0 eV and decreases almost linearly to about 3.5 eV (which is the bulk Mie value) for larger ones (see: Liebsch, A. Electronic Excitations at Metal Surfaces; Plenum: New York, 1997; Figure 3.56; p 138). Similarly in our study, the required electron-detachment energy is about 2.2 eV and the ionization potentials are also away from the plasmon energy (i.e., 5.7-6.0 eV, see Figure 2).
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