John W. Downing
University of Utah
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Featured researches published by John W. Downing.
Pure and Applied Chemistry | 1988
Josef Michl; John W. Downing; T. Karatsu; Allan J. McKinley; G. Poggi; Gregory M. Wallraff; R. Sooriyakumaran; Robert D. Miller
polysilanes r epresent a new class of polymeric materials of considerable theoretical and practical i nterest. Although formally saturated, they absorb in the near UV and undergo rapid photodegradation . After a review of the present understanding of the e lectronic structure of poly(dialkylsi1a nes) as a function of backbone conformation, we summarize their photophysics and describe recent advances in the understanding of their solution
Journal of the Chemical Society, Faraday Transactions | 1994
John W. Downing; Mary Katherine Raymond; V. Balaji; Josef Michl
Information on the potential-energy surfaces of the ground and 1σσ* excited states of oligosilane chains, collected from experimental and theoretical sources, is discussed in terms of electronic structure and the mechanisms of bond and excitation delocalization.
Pure and Applied Chemistry | 1983
Josef Michl; G. J. Radziszewski; John W. Downing; Kenneth B. Wiberg; Frederick H. Walker; Robert D. Miller; Peter Kovacic; Mikolaj Jawdosiuk; V. Bonacic-Koutecky
The infrared spectra of the strained single bond compounds, [2.2.lipropellane, {2.1.1]propellaneand [1.1.1]propellane, andthe vibrational and electronic spectra of the strained bridgehead double bond compounds, adamantene and azahomoadamantene, are reported and discussed.
Chemical Physics | 1977
Erik W. Thulstrup; John W. Downing; Josef Michl
Abstract Linear dichroism in polyethylene, polarization of fluorescence excitation, and magnetic circular dichroism of pyrene and three of its aza derivatives have been measured and used to uncover new electronic transitions and to determine polarization directions. The MCD signs are sensitive to structure. The results, including absolute MCD signs, compare well with π-electron calculations. The effects of systematic incorporation of doubly excited configurations in the CI procedure are investigated. Finally, it is shown that the absolute MCD signs, and in particular, their variation with the location of the aza nitrogen, are readily understood in qualitative terms upon inspection of Huckel MOs, permitting facile predictions for other isomers with-out any computations.
Chemical Physics Letters | 1972
John W. Downing; V. Dvořák; Jaroslav Kolc; A. Manzara; Josef Michl
Abstract Evidence is presented that the second excited state of pleiadene (I) is of doubly excited nature. Such states are of interest in discussions of excited state and ground state reactivities and for further development of calculational methods.
Chemical Physics Letters | 1979
John W. Downing; Josef Michl; Jití Cˇízˇek; Josef Paldus
Abstract A new procedure is proposed for interpolation and extrapolation of functions by a root of a low-degree polynomial. Three examples of the application of the procedure are presented. The rms error in representing SCF surfaces ranges from 2 cal/mole (linear HCN) to 0.23 kcal/mole (C 2V MgH 2 triplet).
Pure and Applied Chemistry | 1987
Josef Michl; Juliusz G. Radziszewski; John W. Downing; Jan Kopecky; Piotr Kaszynski; Robert D. Miller
A survey is given of recent progress in our laboratory in the preparation and spectroscopic characterization of compounds containing highly twisted bridgehead CN and CC double bonds.
Theoretical Chemistry Accounts | 1974
John W. Downing; Josef Michl; Poul Jrgensen; Erik W. Thulstrup
Comparison is presented of energies, oscillator strengths, and polarization directions calculated using the dipole length and dipole velocity formulas for the lowest 4–7ππ* transitions in eight 6π-electron molecules of Cs symmetry using various amounts of CI, from singly excited configurations only (SCI) to complete CI (CCI), and also using the time-dependent Hartree-Fock (TDHF) method. The standard simple PPP approximation was used. For the strongest transitions, SCI and especially TDHF give results in fairly good agreement with CCI. For weaker transitions both SCI and TDHF give similar results, quite different from the CCI solutions. Rational methods for selecting a small number of configurations needed to reproduce correct order of excited states (SECI-1) or a somewhat larger number reproducing correct order, energies, oscillator strengths and polarization directions of transitions (SECI-2) are presented. Both, and particularly the latter, give similar results from both dipole length or dipole velocity formulas when Linderbergs relation is used for matrix elements of the linear momentum operator and in this respect resemble the TDHF and CCI methods for which both formulas necessarily give identical results.
Journal of Molecular Structure-theochem | 1988
Juliusz G. Radziszewski; Charles A. Arrington; John W. Downing; V. Balaji; Gudipati S. Murthy; Josef Michl
Abstract Linear dichroism is observed in the infrared spectra of dimethyl ether, isobutene, 2-butyne, and n-butane dissolved in stretched sheets of ordinary and perdeuterated poly-ethylene. For each observed vibrational band the orientation factor has been determined and related to the transition-moment direction for the vibration, providing information on its symmetry species. For n-butane, the angles of the vibrational transition moment directions in the molecular framework have been derived and compared with the angles calculated at various levels of semiempirical and ab initio theory.
Journal of The Chemical Society-perkin Transactions 1 | 1998
Udo Höweler; John W. Downing; Jörg Fleischhauer; Josef Michl
The LCAO version of the perimeter model with overlap through second order is used to obtain algebraic solutions for the singlet electronic states of the antiaromatic 4N-electron [n]annulenes of Dnh symmetry. The states of these biradicals are classified and their spectroscopic properties derived. General simple results are given for the signs and magnitudes of the A, B and C terms in magnetic circular dichroism. The effects of perturbations that preserve the antiaromatic biradical or biradicaloid character are considered. Other perturbations will be treated in Parts 2 and 3.