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Waves bound

Note that the effect of damping of dm-waves and their nonlinear harmonics as well as free waves depend on the film elasticity. Therefore, one can expect that the resulting phase velocity of the system free waves/bound waves should depend on the characteristics of films. This effect will be studied in further experiments. [Pg.140]

Figure 6.4 shows the spectrum of bound states Eu, in units of E, for f up to 5 for two cases of scattering length, based on the van der Waals quantum defect theory of Gao [9,10]. Panel (a) shows the case of a = oo, where there is a bound state at = 0. The locations of the bound states for a = oo define the boundaries of the bins in which, for any a, there will be one and only one 5-wave bound state, for example, —36.1E < E-ifi < 0 and —249E < F-2,0 < —36.IF. The panel also shows the rotational progressions for each level as increases. The a = oo van der Waals case also follows a rule of 4, where partial waves f = 4,8,... also have a bound state at F = 0. Panel (b) shows how the spectrum changes when a = a, for which the there is a t/-wave level at F = 0. Similar spectra can be calculated for any a. [Pg.228]

Gribakin and Flambaum [14] showed that the near-threshold 5-wave bound state for a van der Waals potential in the limit a fl is modified from the universal form in Equation 6.3 as... [Pg.228]

The properties of bound molecular states near threshold can also be calculated from the general coupled-channels quantum defect method using the properties of the long-range potential. When the energy Eb B) = -h kb B) /i2 x) of the threshold -wave bound state is small, that is, Eb(B) E or kb(B)d 1, then the expression for Eb(B) from the quantum defect method is... [Pg.235]

Gordon R G 1969 Constructing wave functions for bound states and scattering J. Chem. Phys. 51 14-25... [Pg.1004]

In order to illustrate some of the basic aspects of the nonlinear optical response of materials, we first discuss the anliannonic oscillator model. This treatment may be viewed as the extension of the classical Lorentz model of the response of an atom or molecule to include nonlinear effects. In such models, the medium is treated as a collection of electrons bound about ion cores. Under the influence of the electric field associated with an optical wave, the ion cores move in the direction of the applied field, while the electrons are displaced in the opposite direction. These motions induce an oscillating dipole moment, which then couples back to the radiation fields. Since the ions are significantly more massive than the electrons, their motion is of secondary importance for optical frequencies and is neglected. [Pg.1266]

Neuhauser D 1990 Bound state eigenfunctions from wave packets—time -> energy resolution J. Chem. Phys. 932611... [Pg.2327]

Beck M H and Meyer H D 1998 Extracting accurate bound-state spectra from approximate wave packet propagation using the filter-diagonalization method J. Chem. Phys. 109 3730... [Pg.2328]

For bound state systems, eigenfunctions of the nuclear Hamiltonian can be found by diagonalization of the Hamiltonian matiix in Eq. (11). These functions are the possible nuclear states of the system, that is, the vibrational states. If these states are used as a basis set, the wave function after excitation is a superposition of these vibrational states, with expansion coefficients given by the Frank-Condon overlaps. In this picture, the dynamics in Figure 4 can be described by the time evolution of these expansion coefficients, a simple phase factor. The periodic motion in coordinate space is thus related to a discrete spectrum in energy space. [Pg.264]

Until now we have implicitly assumed that our problem is formulated in a space-fixed coordinate system. However, electronic wave functions are naturally expressed in the system bound to the molecule otherwise they generally also depend on the rotational coordinate 4>. (This is not the case for E electronic states, for which the wave functions are invariant with respect to (j> ) The eigenfunctions of the electronic Hamiltonian, v / and v , computed in the framework of the BO approximation ( adiabatic electronic wave functions) for two electronic states into which a spatially degenerate state of linear molecule splits upon bending. [Pg.484]

Eirst decide what the integral equation corresponding to Eq. (6-29) is for the approximate wave function (6-30), then integrate it for various values of y. Report both Y at the minimum energy and Cmin for the Gaussian approximation function. This is a least upper bound to the energy of the system. Your report should include a... [Pg.182]

S, What is the precise value of the least upper bound of the energy for the approximate wave function / e ... [Pg.199]

The values produced may be random and not bounded within any upper or lower limits. This may happen if the boundary conditions on the total wave function are violated. [Pg.193]

Further, if one considers the distance the tensile unloading wave can propagate over the time to fracture f from (8.46), a lower bound criterion for the fragment size can be established... [Pg.291]

Based on the preceding local history, the boundaries at the elastic and plastic wave fronts are characterized by bound surface charges of equal magnitude and opposite sign to the initial piezoelectric states. The polarization in the region behind the plastic wave E3, has magnitude equal to the change... [Pg.100]

As with a high explosive, a fuel-air mixture requires a minimum charge thickness to be able to sustain a detonation wave. Hence, a fully unconfined fuel-air charge should be at least 10 to 13 characteristic-cell sizes thick in order to be detonable. If the charge is bounded by a rigid plane (e.g., the earth s surface) the minimum charge thickness is equal to 5 to 6.5 characteristic-cell sizes (Lee 1983). [Pg.90]

Thepreparadonof resin-bound nitroalkenes via a micro wave-assisted Knoevenagel reacdon of resin-bound nitroacedc acid v/ith aryl and alkyl subsdnited Mdehydes is reported. The potendiil of these resin-bound nitroalkenes for apphcadon in combmatorlM chemistry is demonstratedby a Diels-Alder reacdon v/ith 2,3-dimethylbutadienefScheme 8 9) Iris Mso used for one-pot three-component tandem [4t-2 /[3t-2 reacdons v/ith ethyl vinyl ether and styrene... [Pg.243]

States. Upper and Lower Bounds for Eigenvalues. Accuracy of the Wave Functions.262... [Pg.208]


See other pages where Waves bound is mentioned: [Pg.43]    [Pg.199]    [Pg.36]    [Pg.250]    [Pg.1080]    [Pg.229]    [Pg.506]    [Pg.43]    [Pg.199]    [Pg.36]    [Pg.250]    [Pg.1080]    [Pg.229]    [Pg.506]    [Pg.113]    [Pg.1126]    [Pg.2013]    [Pg.2202]    [Pg.2374]    [Pg.2474]    [Pg.41]    [Pg.229]    [Pg.264]    [Pg.560]    [Pg.178]    [Pg.389]    [Pg.392]    [Pg.134]    [Pg.120]    [Pg.18]    [Pg.99]    [Pg.359]    [Pg.65]    [Pg.100]    [Pg.65]    [Pg.156]    [Pg.206]    [Pg.262]    [Pg.409]    [Pg.90]   
See also in sourсe #XX -- [ Pg.129 , Pg.130 , Pg.134 , Pg.135 , Pg.138 , Pg.139 , Pg.151 , Pg.189 , Pg.199 , Pg.200 , Pg.201 , Pg.202 ]




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