Vibrational calculation

For the BrHh calculations, reviewed below, codes based on Jacobi coordinates and valence coordinates were used to obtain vibrational energies and wave functions. IR transition intensities were obtained for J = 0 to J = 1 transitions using the exact wave functions and the ah initio dipole moment. [Pg.59]

For larger hydrogen-bonded systems, rigorous calculations are far more difficult to carry out, both from the point of view of obtaining full-dimensional potentials and the subsequent quantum vibrational calculations. Reduced dimensionality approaches are therefore often necessary and several chapters in this volume illustrate this approach. With increasing computational power, coupled with some new approaches, it is possible to treat modest sized H-bonded systems in full dimensionality. We have already briefly reviewed the approach we have developed for potentials for the vibrations we have primarily used the code Multimode (MM). The methods used in MM have been reviewed recently [24 and references therein, 25], and so we only give a very brief overview of the method here. [Pg.59]

There are two versions of MM. One, that we refer to as single-reference MM is based on the exact Watson Hamiltonian, which is the Hamiltonian in rectilinear [Pg.59]

Relevant calculations using both versions of MM have been reported for (0H )H20 [21, 26] and H5O2+ [27, 28] and some very recent results will be presented below. Diffusion Monte Carlo calculations, done by and in collaboration with Anne McCoy have also been done on these systems, however, these are not reviewed in detail here. [Pg.60]

The methods discussed above are, in general, concerned only with obtaining the electronic contribution to polarizabilities and hyperpolarizabilities. A complete treatment of the problem requires inclusion of the vibrational and rotational contributions as well. For many experiments at visible frequencies, these effects may be small. For low frequency or static field experiments, however, these effects have been shown to be as large or larger than the electronic effects themselves.Bishop and Kirtman developed a general approach for calculating the vibrational contributions for polyatomic systems. A recent overview of this subject can be found in the review by Kirtman and Champagne. [Pg.273]

Once the vibration calculation completes, you can analy/eand display Ihe results by using Vibrational Spectrum menu item. [Pg.124]

One type of single point calculation, that of calculating vibrational properties, is distinguished as a vibrations calculation in HyperChem. A vibrations calculation predicts fundamental vibrational frequencies, infrared absorption intensities, and normal modes for a geometry optimized molecular structure. [Pg.16]

Single-point, geometry optimization, molecular dynamics and vibration calculations are all available with either ab initio or semi-empirical SCFmethods. After obtaining a wavefunction via any of... [Pg.120]

Note You cannot use the Extended Hiickel method or any one of the SCFmethods with the Cl option being turned on for geometry optimizations, molecular dynamics simulations or vibrational calculations, in the current version of HyperChem. [Pg.122]

A vibrations calculation is the first step of a vibrational analysis. It involves the time consuming step of evaluating the Hessian matrix (the second derivatives of the energy with respect to atomic Cartesian coordinates) and diagonalizing it to determine normal modes and harmonic frequencies. For the SCFmethods the Hessian matrix is evaluated by finite difference of analytic gradients, so the time required quickly grows with system size. [Pg.124]

HyperChem computes the Hessian using numerical second derivative of the total energy with respect to the nuclear positions based on the analytically calculated first derivatives in ab initio methods and any of the semi-empirical methods, except the Extended Hiickel. Vibration calculations in HyperChem using an ab initio method may take much longer than calculations using the semi-empirical methods. [Pg.332]

Benzene has often been used as a test system for vibrational calculations using a variety of different electronic structure algorithms. The molecule exhibits regular hexagonal planar symmetry with six carbon atoms joined by a bonds and six remaining p-orbitals which overlap to form a delocalised n electron over all six carbon atoms. Table 1 shows comparisons of several different methods for benzene. [Pg.34]

ANHARMONICIT Y OF THE CH STRETCHING MODES 3.2.1. Electronic and vibrational calculations... [Pg.406]

The most isotope sensitive motions in molecules are the vibrations, and many thermodynamic and kinetic isotope effects are determined by isotope effects on vibrational frequencies. For that reason it is essential that we have a thorough understanding of the vibrational properties of molecules and their isotope dependence. To that purpose Sections 3.1.1, 3.1.2 and 3.2 present the essentials required for calculations of vibrational frequencies, isotope effects on vibrational frequencies (and by implication calculation of isotope effects on thermodynamic and kinetic properties). Sections 3.3 and 3.4, and Appendices 3.A1 and 3.A2 treat the polyatomic vibrational problem in more detail. Students interested primarily in the results of vibrational calculations, and not in the details by which those results have been obtained, are advised to give these sections the once-over lightly . [Pg.55]

Bemath, P. F. Spectra of Atoms and Molecules. 2nd Ed. Oxford University Press, Oxford (2005). Miyazawa, T. Symmetrization of secular determinant for normal vibration calculation. J. Chem. Phys. 29, 246 (1958). [Pg.76]

Detailed vibrational calculations (Bottinga, 1968 Becker, 1971 Kieffer, 1982) as well as accurate experiments (Clayton et al., 1989 Chiba et al., 1989, and references therein) and semiempirical generalizations (Zheng, 1991, 1993a,b) have been made since the work of Urey (1947) and ensure satisfactory knowledge of the fractionation properties of minerals and water and mineral-mineral... [Pg.772]

Figure 11,31 Oxygen isotopic fractionation between calcite and diopside as obtained from equations 11.131 to 11.133. Experimental data points are from Chiba et al. (1989). Dotted line indications from vibrational calculations following Kielfer s (1982) procedure. From Clayton and Kielfer (1991), reprinted with kind permission of The Geochemical Society, Pennsylvania State University, University Park, Pennsylvania.

$Figure 11,31 Oxygen isotopic fractionation between calcite and diopside as obtained from equations 11.131 to 11.133. Experimental data points are from Chiba et al. (1989). Dotted line indications from vibrational calculations following Kielfer s (1982) procedure. From Clayton and Kielfer (1991), reprinted with kind permission of The Geochemical Society, Pennsylvania State University, University Park, Pennsylvania.$

Watanabe, H., Hayazawa, N., Inouye, Y, and Kawata, S. 2005. DFT vibrational calculations of rhodamine 6G adsorbed on silver Analysis of tip-enhanced Raman spectroscopy. J. Phys. Chem. B 109 5012-20. [Pg.271]

The normal mode calculation was used to elucidate the rotational isomerization equilibrium of the [C4CiIm]X liquids. In the wave number region near 800-500 cm, where ring deformation bands are expected, two Raman bands appeared at —730 cm and —625 cm in the [C4C4lm]Cl Crystal (1). In the [C4CiIm]Br these bands were not found. Here instead, another couple of bands appeared at —701 and —603 cm T To assist the interpretation of the spectra, the normal modes of vibrations calculated by Hamaguchi et al. [50] are shown in Figure 12.8. [Pg.318]

Fig. 7. The potential energy surface for the two Eg normal modes of vibration calculated at the CASSCF(4,5)/TZVPP level of theory.

Fig. 10. Energy spectrum for the lower electronic states of Cr(H20)l+, along the path of the normal mode of vibration, calculated using the CASSCF(4,5) method and the TZVPP basis set.

If chloroform (trichloromethane) exhibits an infrared peak at 3 018 cm-1 due to the C-H stretching vibration, calculate the wavenumber of the absorption band corresponding to the C D stretching vibration in deuterochloroform (experimental value 2253 cm-1). [Pg.186]

Normal vibration calculations, if based on a correct structure and correct potential field, would supposedly permit a unique correlation to be made between predicted and observed absorption bands. In most cases this ideal situation is far from being achieved in the study of high polymer spectra. More usually the structure and force field are to some extent unknown, or normal mode calculations are not available, so that other methods must be used in order to establish the origin of bands in the spectrum. Even if complete calculations were available it would be desirable to check their predictions by means other than a comparison of observed and predicted frequency values. One method of doing so is by studying isotopically substituted molecules, and the most useful case is that in which deuterium is substituted for hydrogen. [Pg.91]

The infrared active v (CH2), v (CH2), 8 (CH2), and yr (CH2) fundamentals can be readily assigned as a result of the extensive spectroscopic studies on hydrocarbons which have been undertaken [Sheppard and Simpson (795)]. In addition, because of the polarized radiation studies on single crystals of normal paraffins [Krimm (95)], it is possible to assign uniquely the components of the doublets found in the spectrum for these bands to symmetry species. Similarly, the Raman active va(CH. ), vs(CH2), (CHg), v+ (0), and v+ (n) fundamentals can be unambiguously assigned, the latter two on the basis of normal vibration calculations... [Pg.109]

Vibration (calculates the vibrational motions of selected atoms)... [Pg.305]

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