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Vibrational anharmonicity energy

In the vibrational treatment we assumed, as usually done, that the Born-Oppenheimer separation is possible and that the electronic energy as a function of the internuclear variables can be taken as a potential in the equation of the internal motions of the nuclei. The vibrational anharmonic functions are obtained by means of a variational treatment in the basis of the harmonic solutions for the vibration considered (for more details about the theory see Pauzat et al [20]). [Pg.407]

Figure 1.4 The very anharmonic energy levels of the C6H6 - Ar stretch motion (cf. Figure 0.3) (adapted from Neusser, Sussman, Smith, Riedle, and Weber, 1992). The computed values of the rotational constant Bv [the coefficient of 1(1+1) in the expression for the energy eigenvalues] are given in the figure, as are the vibrational spacings. Figure 1.4 The very anharmonic energy levels of the C6H6 - Ar stretch motion (cf. Figure 0.3) (adapted from Neusser, Sussman, Smith, Riedle, and Weber, 1992). The computed values of the rotational constant Bv [the coefficient of 1(1+1) in the expression for the energy eigenvalues] are given in the figure, as are the vibrational spacings.
In the hydrate lattice structure, the water molecules are largely restricted from translation or rotation, but they do vibrate anharmonically about a fixed position. This anharmonicity provides a mechanism for the scattering of phonons (which normally transmit energy) providing a lower thermal conductivity. Tse et al. (1983, 1984) and Tse and Klein (1987) used molecular dynamics to show that frequencies of the guest molecule translational and rotational energies are similar to those of the low-frequency lattice (acoustic) modes. Tse and White (1988) indicate that a resonant coupling explains the low thermal conductivity. [Pg.100]

For diatomic molecules, corrections can be made for the assumption used in the derivation of the rotational partition function that the rotational energy levels are so closely spaced that they can be considered to be continuous. The equations to be used in making these corrections are given in Appendix 6. Also given are the equations to use in correcting for vibrational anharmonicity and nonrigid rotator effects. These corrections are usually small.22... [Pg.32]

A more precise measurement of local sample temperature is made possible by the anharmonicity of the crystal vibrational potential energy. Phonon-phonon interactions that reduce individual phonon lifetimes, phonon softening, and thermal expansion give rise to increasing peak width and a change in peak frequency... [Pg.501]

The heat capacity (C ) and heat conductivity (A) of crystals depend respectively on the vibrational density of states weighted by a Boltzmann s distribution factor and the anharmonic terms in the vibrational potential energy. C has been found to be in the range 0.100 to 0,117 cal./g./°C between 100—250 °C for crystals as widely varying in lattice geometry as mercuric fulminate, silver azide and lead azide 62). This is... [Pg.41]

Ab initio constmction of such anharmonic energy surfaces for quite complicated systems has been feasible for some years, thanks to increased compnting power and veiy time-efficient quantum-mechanical software. Many years before such calculations became possible, however, Marcus (1959, 1960, 1965) showed that, by treating the internal vibrational modes of D and and A and A , as symmetrised classical harmonic... [Pg.226]

The calculation of third and fourth derivatives is attractive for two reasons these are the quantities needed in the lowest-order treatment of vibrational anharmonicities, and a quartic surface is the simplest to exhibit a double minimum, i.e. the simplest model of a reaction surface. Moccia (1970) did apparently first consider the SCF third derivative problem. A detailed derivation of SCF and MCSCF third derivatives was given by Pulay (1983a) independently, Simons and J )rgensen (1983) also considered the calculation of MCSCF third, and even fourth, derivatives in a short note. As pointed out in Section II, third derivatives of the energy require only the first derivatives of the coefficients, and are thus computationally attractive. By contrast, fourth derivatives require the solution of the second-order CP MCSCF equations. The only computer implementation so far is that of Gaw etal.( 984) for closed shells, although the detailed theory has been worked out for the MCSCF case... [Pg.268]

To calculate n E-E, the non-torsional transitional modes have been treated as vibrations as well as rotations [26]. The former approach is invalid when the transitional mode s barrier for rotation is low, while the latter is inappropriate when the transitional mode is a vibration. Harmonic frequencies for the transitional modes may be obtained from a semi-empirical model [23] or by performing an appropriate normal mode analysis as a function of the reaction path for the reaction s potential energy surface [26]. Semiclassical quantization may be used to determine anharmonic energy levels for the transitional modes [27]. [Pg.1016]


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See also in sourсe #XX -- [ Pg.204 , Pg.205 , Pg.213 , Pg.216 ]




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Anharmonicity

Energy vibrational

Vibration energy

Vibrational anharmonicities

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