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MA Mekhtiev

Publications and source records attributed to MA Mekhtiev.

3 recordsLinked to original sources

Contact Transformations and Determinable Parameters in Spectroscopic Fitting Hamiltonians.

In recent least-squares fits of torsion-rotation spectra of acetaldehyde and methanol it was found possible to adjust more fourth-order parameters than would be expected from traditional contact-transformation considerations. To investigate this discrepancy between theory and practice we have carried out numerical fitting experiments on the simpler three-dimensional (three-Eulerian-angle) asymmetric rotor problem, using J </= 20 unitless energy levels generated artificially from a full orthorhombic Hamiltonian with quadratic through octic operators in the angular momentum components. Results are analyzed using the condition number kappa of the least-squares matrix, which is a measure of its invertibility in the presence of round-off and other errors. When kappa is very large, parameters must be removed from the fit until kappa becomes acceptably small, corresponding to procedures which lead to reduced Hamiltonians in molecular spectroscopy. We find that under certain circumstances kappa can be decreased to an acceptable level for Hamiltonians which are only partially reduced when compared to Watson A and S reductions. Some insight into this behavior is obtained from classical mechanics and from the concept of delayed contact transformations. Transferring this numerical and algebraic understanding to the more complicated four-dimensional methyl-top internal rotor problem supports the empirical observation that presently existing data sets for methanol and acetaldehyde are most efficiently fit using partially reduced Hamiltonians and further suggests that expanding the methanol data set to transitions involving levels of higher J, K, and v(t) would favor even more strongly the use of partially reduced fourth-order Hamiltonians.

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Linestrengths of Torsion-Rotation Transitions of Methanol for J </= 22, K </= 14, and upsilont </= 2 from Hamiltonian-Based Calculations.

Linestrengths have been obtained for methanol based on matrix elements of the dipole moment operator evaluated in a set of torsion-rotation eigenfunctions. The latter were obtained from the parameters and effective Hamiltonian giving the best spectral fit available for a data set containing J </= 20, K </= 14, and upsilont </= 1 microwave and far infrared transitions. The dipole moment function was represented as a Fourier expansion in the torsional angle gamma. Values for the permanent components µa and µb were obtained from experiment; values for their cos 3gamma variation and for the sin 3gamma variation of µc were obtained from quantum chemistry molecular orbital calculations. The approach described allows calculation of the linestrength for any transition which satisfies the general selection rule A1 left and right arrow A2 or E left and right arrow E. A complete set of such linestrengths for all methanol torsion-rotation transitions involving levels with J </= 22, K </= 14, and upsilont </= 2, and with intensities and frequencies above the rather small cutoff limits of 10(-6) D2 and 1 kHz, respectively, together with individual contributions from the permanent and gamma-varying dipole moment components, have been tabulated and are available on request (ftp.monash.edu.au/pub/chem/1998a). Copyright 1999 Academic Press.

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Some Properties and Uses of Torsional Overlap Integrals

The first diagonalization step in a rho-axis-method treatment of methyl-top internal rotation problems involves finding eigenvalues and eigenvectors of a torsional Hamiltonian, which depends on the rotational projection quantum number K as a parameter. Traditionally the torsional quantum number vt = 0, 1, 2&middot;&middot;&middot;is assigned to eigenfunctions of given K in order of increasing energy. In this paper we propose an alternative labeling scheme, using the torsional quantum number vT, which is based on properties of the K-dependent torsional overlap integrals . In particular, the quantum number vT is assigned in such a way that torsional wavefunctions |vT, K> vary as slowly as possible when K changes by unity. Roughly speaking, vT = vt for torsional levels below the barrier, whereas vT is more closely related to the free-rotor quantum number for levels above the barrier. Because of the latter fact, we believe vT will in general be a physically more meaningful torsional quantum number for levels above the barrier. The usefulness of overlap integrals for qualitative prediction of torsion-rotation band intensities and for rationalizing the magnitudes of perturbations involving some excitation of the small-amplitude vibrations in an internal rotor problem is also discussed. Copyright 1998 Academic Press. Copyright 1998Academic Press

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