2001
DOI: 10.1006/jmsp.2000.8275
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The General Harmonic Force Field of Methyl Chloride

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Cited by 22 publications
(7 citation statements)
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“…Mössbauer-based fractionation models are based on an extension of Equations (4) and (5) (Bigeleisen and Mayer 1947), which relate to either sums of squares of vibrational frequencies or a sum of force constants. In the Polyakov (1997) (Black and Law 2001) and ab initio vibrational frequencies for methyl chloride, 12 C 1 H 3 35 Cl. Ab initio frequencies are calculated with GAMESS, using the Hartree-Fock method and 6-31G(d) basis set.…”
Section: Theoretical Applications Of Mössbauer Spectroscopymentioning
confidence: 99%
“…Mössbauer-based fractionation models are based on an extension of Equations (4) and (5) (Bigeleisen and Mayer 1947), which relate to either sums of squares of vibrational frequencies or a sum of force constants. In the Polyakov (1997) (Black and Law 2001) and ab initio vibrational frequencies for methyl chloride, 12 C 1 H 3 35 Cl. Ab initio frequencies are calculated with GAMESS, using the Hartree-Fock method and 6-31G(d) basis set.…”
Section: Theoretical Applications Of Mössbauer Spectroscopymentioning
confidence: 99%
“…Much attention has been given to a description of harmonic [33][34][35][36][37][38][39][40] and anharmonic 9,41-46 force fields, both empirically and using ab initio methods. The latest work by Black and Law 40 employed spectroscopic data from ten isotopomers of methyl chloride to produce an empirical harmonic force field incorporating the most up to date treatment of anharmonic corrections. These were largely based on a complete set of empirical anharmonicity constants derived from a joint local mode and normal mode analysis of 66 vibrational energy levels in the region of 700-16 500 cm −1 , 45 and follow-up work in a similar vein by Law.…”
Section: Introductionmentioning
confidence: 99%
“…Wavenumber a Reference Differently from the parent species CH 3 Cl (C 3v group), in which the carbonhalogen bond lies on the symmetry axis, the a-axis of the principal inertia system of CH 2 DCl is slightly rotated with the respect to the C -Cl bond because of the different center of mass. Replacing one hydrogen atom with deuterium causes the permanent dipole moment (µ = 1.870 D for CH 3 Cl [32]) to be distributed along two components; based on geometric considerations [33], and assuming that the total dipole moment does not change among the isotopologues, one can estimate µ a = 1.868 D and µ b = 0.076 D for CH 2 DCl. The rotational energy of CH 2 DCl can be modeled by using the standard semirigid Hamiltonian for an asymmetric rotor with a non-vanishing nuclear spin:…”
Section: Symmetry Mode Descriptionmentioning
confidence: 99%