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Diatoms, 341 energy

Vibrational spectroscopy Calculation of diatomic energy level spacings, isotope shifts... [Pg.83]

Figure 5.4 Homonuclear diatomic energy curve in dimensionless units... Figure 5.4 Homonuclear diatomic energy curve in dimensionless units...
The depth of understanding of V-V, V-T, and V-R, relaxation in atom-diatom collisions at low densities is profound. " The advent of state-to- state experiments and of quantum, semiclassical, and classical calculations has provided a wealth of information. Stochastic approaches, which are still under development for polyatomic sys-tems should mimic the essential features of thermally averaged atom-diatom energy transfer when applied to these simple systems. The friction is essentially the characteristic of kinetic energy relaxation. The energy diffusion equation of the energy probability density tr(E, t) is... [Pg.420]

The DIM method is most commonly employed as a semi-empirical technique. The fragment Hamiltonian matrices are usually related to atomic and diatomic energies by making various approximations for the overlap matrices. Both the form of the DIM equation and the chosen set of PBF must be sufficient to account for all the qualitative features of the system being studied. Under such circumstances the approach may offer acceptable accuracy for modest computational effort. Given the input of experimental and accurate theoretical data for the fragments, it is not unreasonable to suppose that the method can yield results comparable to those from larger... [Pg.372]

Definition. Let us consider a given diatomic energy function Um(R) obtained from quantum-chemical calculations or experimental data, where m enumerates electronic states. We assume that Um(R) has at least one minimum at R = Re. Then the nth-order diatomic force constant 4m) for the mth electronic state is defined as follows ... [Pg.168]

If the diatomic overlap is retained in evaluating the diatomic energies then (44) becomes... [Pg.167]

Table 3.1 Carbon-Carbon Bond Strength in Various Substrates in Terms of Diatomic Energy (kJ/mol) ... Table 3.1 Carbon-Carbon Bond Strength in Various Substrates in Terms of Diatomic Energy (kJ/mol) ...
Table 3.6 Carbon-Carbon Bond Strengths in Substrates with Zigzag Edges. Expressed by Diatomic Energy (kj/mol)... Table 3.6 Carbon-Carbon Bond Strengths in Substrates with Zigzag Edges. Expressed by Diatomic Energy (kj/mol)...
Abstract, In this paper I give an overview of the current status of knowledge of the four-body potential energy function and dynamics of the HF dimer. The discussion of potential energy functions includes both single-center expansions and multi-site functions. The discussion of d)mamics includes both intramolecular processes of the van der Waals dimer and diatom-diatom energy transfer collisions. [Pg.159]

Figure 17.8 Relaxed triangular plot in hyperspherical coordinates (dimensionless) of the CHIPRI PES for groxmd state H3. Solid contours are at intervals of 0.005 Eh, starting at the separated atom-diatom energy. Indicated are the three symmetry-related collinear saddle points (solid dots) and the conical intersection (open circles). Diametrically opposed to the former are the atom-united-atom of H2 limits and, nearby, the H- -H2 vdW minima. Figure 17.8 Relaxed triangular plot in hyperspherical coordinates (dimensionless) of the CHIPRI PES for groxmd state H3. Solid contours are at intervals of 0.005 Eh, starting at the separated atom-diatom energy. Indicated are the three symmetry-related collinear saddle points (solid dots) and the conical intersection (open circles). Diametrically opposed to the former are the atom-united-atom of H2 limits and, nearby, the H- -H2 vdW minima.
Abstract Some previous results of the present author are combined in order to develop a Hermitian version of the Chemical Hamiltonian Approach. In this framework the second quantized Bom-Oppenheimer Hamiltonian is decomposed into one- and two-center components, if some finite basis corrections are omitted. (No changes are introduced into the one- and two-center integrals, while projective expansions are used for the three- and four-center ones, which become exact only in the limit of complete basis sets.) The total molecular energy calculated with this Hamiltonian can then presented as a sum of the intraatomic and diatomic energy terms which were introduced in our previous chemical energy component analysis scheme. The corresponding modified Hartree-Fock-Roothaan equations are also derived they do not contain any three- and four-center integrals, while the non-empirical character of the theory is conserved. This scheme may be useful also as a layer in approaches like ONIOM. [Pg.35]

Although a diatomic molecule can produce only one vibration, this number increases with the number of atoms making up the molecule. For a molecule of N atoms, 3N-6 vibrations are possible. That corresponds to 3N degrees of freedom from which are subtracted 3 translational movements and 3 rotational movements for the overall molecule for which the energy is not quantified and corresponds to thermal energy. In reality, this number is most often reduced because of symmetry. Additionally, for a vibration to be active in the infrared, it must be accompanied by a variation in the molecule s dipole moment. [Pg.57]

The interaction energy can be written as an expansion employing Wigner rotation matrices and spherical hamionics of the angles [28, 130], As a simple example, the interaction between an atom and a diatomic molecule can be expanded hr Legendre polynomials as... [Pg.208]

These results do not agree with experimental results. At room temperature, while the translational motion of diatomic molecules may be treated classically, the rotation and vibration have quantum attributes. In addition, quantum mechanically one should also consider the electronic degrees of freedom. However, typical electronic excitation energies are very large compared to k T (they are of the order of a few electronvolts, and 1 eV corresponds to 10 000 K). Such internal degrees of freedom are considered frozen, and an electronic cloud in a diatomic molecule is assumed to be in its ground state f with degeneracy g. The two nuclei A and... [Pg.405]

The energy of a diatomic molecule can be divided into translational and internal contributions = (/ik) /(2A7)... [Pg.405]

The direct dissociation of diatomic molecules is the most well studied process in gas-surface dynamics, the one for which the combination of surface science and molecular beam teclmiques allied to the computation of total energies and detailed and painstaking solution of the molecular dynamics has been most successful. The result is a substantial body of knowledge concerning the importance of the various degrees of freedom (e.g. molecular rotation) to the reaction dynamics, the details of which are contained in a number of review articles [2, 36, 37, 38, 39, 40 and 41]. [Pg.906]

Figure A3.9.8. An elbow potential energy surface representing the dissociation of a diatomic in two dimensions-the molecular bond lengdi and tlie distance from the molecule to the surface. Figure A3.9.8. An elbow potential energy surface representing the dissociation of a diatomic in two dimensions-the molecular bond lengdi and tlie distance from the molecule to the surface.
There usually is rotational motion accompanying the vibrational motion, and for a diatomic, the energy as a fiuictioii of the rotational qiiantum iiumber, J, is... [Pg.1153]

As an illustrative example, consider the vibrational energy relaxation of the cyanide ion in water [45], The mechanisms for relaxation are particularly difficult to assess when the solute is strongly coupled to the solvent, and the solvent itself is an associating liquid. Therefore, precise experimental measurements are extremely usefiil. By using a diatomic solute molecule, this system is free from complications due to coupling... [Pg.1173]


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Diatomic energies

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