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  • 1985-1989  (9)
Material
Years
Year
  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 93 (1989), S. 5079-5087 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 6658-6666 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An approach is presented and demonstrated for determining predissociation lifetimes of small molecules in the vapor phase at room temperature through measurement of resonance Raman depolarization ratios. Depolarization ratios for low-pressure CS2 vapor have been measured using ten excitation wavelengths between 1995 and 2001 A(ring), spanning one of the strongest vibrational features of the S3←S0 electronic transition. The excitation wavelengths are obtained by anti-Stokes Raman shifting in H2 the fourth harmonic of a Nd:YAG laser and the second harmonic of a YAG-pumped dye laser. The Raman depolarization ratio ρ(I⊥/I(parallel)) varies from less than 0.4 with excitation on the high-frequency side of the vibronic band to nearly 0.6 on the low-frequency side. Numerical simulation of the depolarization dispersion curve using literature values for the rotational constants shows that this behavior can be attributed straightforwardly to partially selective excitation of initial J states for which the S3 predissociation lifetime is either long or short relative to rotational periods. The best fit between the experimental and calculated depolarization dispersion curves is obtained with a homogeneous linewidth of 6 cm−1 (excited state lifetime 0.9 ps). The relevance of this result to measurements of dissociation times through photofragment anisotropy analysis is discussed.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 1876-1886 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Complete resonance Raman spectra, including absolute cross sections, have been measured for CS2 in cyclohexane using four excitation wavelengths from 223 to 204 nm, on resonance with the strongly allowed S3←S0 electronic transition. Absolute intensities have also been measured in CS2 vapor using 200 nm excitation. These total Raman cross sections, together with the Rayleigh cross sections calculated from the Kramers–Kronig transform of the absorption spectrum, are used to determine the homogeneous linewidth Γ for the electronic transition under the assumption that the solvent induced broadening may be partitioned into a static, inhomogeneous part and a very rapidly modulated, homogeneous component. Γ is found to be ∼13 cm−1 in the vapor and ∼200 cm−1 in cyclohexane solution, indicating that homogeneous broadening is responsible for much of the increase in spectral breadth between vapor and solution phases. Direct modeling of the solution phase absorption spectrum and the intensities of the lower lying Raman transitions gives a best fit to the absolute cross sections with a somewhat smaller Γ of ∼115 cm−1, probably due to the approximate nature of the model employed for the highly anharmonic excited state potential surface. The possible importance of solvent "memory'' effects (finite solvent correlation time) on the electronic spectral broadening is discussed.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 87 (1987), S. 2116-2121 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The effect of the finite time for resonance Raman scattering on Raman depolarization ratios is evaluated. Partial depolarization of the resonance Raman emission will occur if the scatterers can rotate during the time interval between the absorption and emission steps. Equations are derived which express the depolarization ratio in terms of Fourier transforms of the usual time-dependent vibrational overlap multiplied by a rotational correlation function. Particularly simple results are obtained in the limit of severe inhomogeneous broadening of the electronic transition. The effect of the finite resonance scattering time on the line shape of the resonance Raman transition is also discussed.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 86 (1987), S. 5146-5155 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Ultraviolet fluorescence upconversion gating has been used to measure the fluorescence anisotropy of aniline in four hydrocarbon and alcoholic solvents. The deconvoluted anisotropy decay time of 1.2 ps in isopentane is only about a factor of 2 longer than calculated for free rotation of collision-free molecules, and increasing the solvent viscosity by a factor of 15 by going from isopentane to hexadecane increases the rotational relaxation time by only another factor of 2. These results imply that the orientational motion of electronically excited aniline in hydrocarbons may be significantly nondiffusive and that unhindered inertial rotation through large angles may be possible. The experimental anisotropy decays do, however, differ significantly from those calculated for completely unhindered free rotation. The anisotropy decays much more slowly in methanol and sec-butanol than in the hydrocarbons, presumably due to dipole–dipole and/or hydrogen bonding interactions in the hydroxylic solvents. The rotational relaxation of N,N-dimethylaniline is slower than that of aniline in hydrocarbon solvents but faster in methanol, perhaps reflecting reduced hydrogen bonding. Fluorescence anisotropy decays of 4-cyclohexylaniline and 2,4,6-tri-tert-butylaniline have also been examined in order to estimate the true initial rotationless anisotropy [r(0)] for aniline.
    Type of Medium: Electronic Resource
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  • 6
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 6301-6314 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A theoretical treatment of time-resolved fluorescence polarization and two time-resolved four-wave mixing processes (polarization spectroscopy and transient gratings) from a thermal ensemble of free symmetric top rotors is presented. Time-dependent signals are calculated for both parallel and perpendicular transitions at low and high temperatures. At high J, both the fluorescence anisotropies and the nonlinear signals exhibit transients near time zero which level out to essentially constant values within several average rotational periods. These transients, which represent rigid-body rotational motion in a classical picture, arise in a quantum mechanical treatment from interferences between different intermediate rotational states that are coupled to the same pair of initial and final states. The nonlinear signals are sensitive not only to rotational dynamics but also to the total dephasing rates between the final pairs of coupled levels and to effects of selective phase matching. The relevance of these short-time effects for designing and interpreting experiments to probe rotational dynamics of large molecules is discussed.
    Type of Medium: Electronic Resource
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  • 8
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The sensitivity of absolute resonance Raman cross sections to the excited state homogeneous width is used to examine whether the electronic spectral breadth induced by the β-ionone ring of retinal is primarily a homogeneous or an inhomogeneous effect. Resonance Raman intensities have been measured for both all-trans retinal and its 5,6-dihydro analog. The dihydro analog has a structured absorption spectrum because the broadening effect of the C6–C7 bond is lost when the π system does not extend into the ionone ring. While the two molecules have similar relative Raman intensities, the absolute cross sections are about a factor of two lower in all-trans retinal, indicating that the "effective homogeneous linewidth'' is significantly larger in all-trans retinal than in the dihydro analog. Calculations carried out to model both the absorption spectra and the resonance Raman intensities require an effective homogeneous linewidth that is more than twice as large for all-trans retinal (∼1200 cm−1) as for the 5,6-dihydro analog (∼500 cm−1). The additional width is most simply attributed to Franck–Condon activity in the C6–C7 torsional degree of freedom; however, no intense resolved lines are observed in the Raman spectrum between 20 and 800 cm−1. The torsional modes involved must have very low ground-state frequencies and may be observable only through their contribution to the apparent Rayleigh and Raman linewidths.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 83 (1985), S. 5000-5006 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The sensitivity of resonance Raman cross sections to the excited state homogeneous width is exploited to separate the homogeneous and inhomogeneous contributions to the optical absorption linewidth in trans-stilbene. Absolute Raman cross sections have been measured using excitation at 356, 299, 282, and 266 nm, and calculations have been performed to model the intensities of the eleven strongly Raman-active modes as well as the absorption spectrum. A simple analysis neglecting explicit temperature effects requires a homogeneous Lorentzian linewidth (Γ) of 310 cm−1 and an inhomogeneous Gaussian distribution of zero–zero energies with a standard deviation (θ) of 500 cm−1. Consideration of thermal excitation in the lowest-frequency single-bond torsional mode significantly improves the fit to the experimental absorption by broadening the spectrum asymmetrically to higher energies, while allowing Γ and θ to be reduced to 120 and 450 cm−1, respectively. The spectral broadening generated by thermal excitation of ground-state torsional modes thus contributes significantly to the homogeneous linewidth in trans-stilbene. The relatively large effective homogeneous width at room temperature is consistent with the low Raman intensity in the ∼200 cm−1 C=C–φ bend compared with the prominence of this vibration in resolved low-temperature electronic spectra.
    Type of Medium: Electronic Resource
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