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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 779-785 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the laser photolysis/laser-induced fluorescence (LIF) "pump-and-probe" technique, the dynamics of H atom formation in the photodissociation of CH3–CF2Cl (HCFC-142b) after excitation at 193 nm and the Lyman-α wavelength were studied under collision-free conditions in the gas-phase at room temperature. The H atoms produced were detected by (2p2P←1s2S)-LIF using tunable narrow-band Lyman-α laser radiation (λLα(approximate)121.6 nm) generated by resonant third-order sum-difference frequency conversion of pulsed dye laser radiation. In the VUV photodissociation experiments the Lyman-α laser radiation was used both to photodissociate the parent molecules and to detect the produced nascent H atoms via laser induced fluorescence. The following quantum yields ΦH for H atom formation were determined by a photolytic calibration method: ΦH(193 nm)=(0.06±0.02) and ΦH(Lα)=(0.53±0.12). From the measured H atom Doppler profiles the average H atom kinetic energy was determined to be ET(193 nm)=(51±10) kJ/mol and ET(Lα)=(72±4) kJ/mol, respectively. © 1997 American Institute of 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 106 (1997), S. 1359-1366 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The gas-phase dissociation dynamics of CH3Cl, CH2Cl2, and CHCl3 after photoexcitation at the Lyman-α wavelength (121.6 nm) were studied under collision-free conditions at room temperature. Narrow-band tunable Lyman-α laser radiation (λLα(approximate)121.6 nm) was generated by resonant third-order sum-difference frequency conversion of pulsed-dye-laser radiation and used both to photodissociate the parent molecules and to detect the nascent H atom products via (2p2P←1s2S) laser induced fluorescence. Absolute H atom quantum yields ΦH(CH3Cl)=(0.53±0.05), ΦH(CH2Cl2)=(0.28±0.03), and ΦH(CHCl3)=(0.23±0.03) were determined employing a photolytic calibration method where the Lyman-α photolysis of H2O was used as a reference source of well-defined H atom concentrations. H atom Doppler profiles were measured for all chlorinated methanes. In the case of CH3Cl the line shapes of the profiles indicate a pronounced bimodal translational energy distribution suggesting the presence of two H atom formation mechanisms leading to a markedly different H atom translational energy release. The observed "slow" component of the H atom translational energy distribution corresponds to an average kinetic energy of (55±5) kJ/mol, while the "fast" component leads to an average kinetic energy of (320±17) kJ/mol. The relative branching ratio between the "fast" and the "slow" H atom channel was determined to be (0.71±0.15). For CH2Cl2 and CHCl3 no bimodal translational energy distributions were observed. Here the translational energy distributions could each be well described by a single Maxwell–Boltzmann distribution, corresponding to an average translational energy of (81±9) kJ/mol and (75±4) kJ/mol, respectively. © 1997 American Institute of Physics.
    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 106 (1997), S. 9563-9569 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the laser photolysis–laser-induced fluorescence "pump–probe" technique, the gas-phase dissociation dynamics of HNCO(X˜ 1A)+hν→H+NCO and DNCO(X˜ 1A)+hν→D+NCO after photoexcitation at the Lyman-α wavelength were studied under collision-free conditions at room temperature. In the vacuum ultraviolet photodissociation experiments narrow band tunable Lyman-α laser radiation (λ(approximate)121.4–121.6 nm) was used both to photodissociate the parent molecules and to detect the produced nascent H and D atom products via (2p 2P←1s 2S) laser induced fluorescence. The following quantum yields ΦH–D for H–D atom formation were determined by a photolytic calibration method: ΦH=(0.62±0.15) and ΦD=(0.51±0.17). For HNCO and DNCO the measured H–D atom Doppler line shapes can be well described by a single Gaussian function, which corresponds to a statistical Maxwell–Boltzmann-like distribution of the translational energy. From the measured H and D atom Doppler profiles the average H and D atom kinetic energy was determined to be ET(H)=(137±10) kJ/mol and ET(D)=(115±4) kJ/mol, respectively. The average kinetic energies were found to be in reasonable agreement with results from simple statistical calculations in which it is assumed that H–D atoms are produced in combination with NCO in the ground electronic state (X˜ 2Π). A dissociation mechanism is suggested in which H–D atom formation proceeds via a statistical unimolecular decay of a hot H–DNCO intermediate formed by a radiationless transition of the optically excited bound H–DNCO state to a lower-lying dissociative state. © 1997 American Institute of Physics.
    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 106 (1997), S. 4436-4447 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the laser photolysis/laser-induced fluorescence (LP/LIF) pump–probe technique, the gas phase photodissociation dynamics of room temperature DNCO were studied at photolysis wavelengths of 193 and 248 nm. D atoms produced via DNCO (X˜ 1A)+hν→D(2S)+NCO(X˜ 2Π) were detected by (2p 2P←1s 2S)-LIF using tunable narrow-band Lyman-α laser radiation (λLα(approximate)121.5 nm) generated by resonant third-order sum-difference frequency conversion of pulsed dye laser radiation. By means of a photolytic calibration method absolute cross sections for the direct photochemical D atom formation were measured to be σD(193 nm)=(5.5±0.5)×10−20 cm2 molecule−1 and σD(248 nm)=(1.2±0.2)×10−21 cm2 molecule−1. For the wavelength of 193 nm, the measurement of the optical absorption cross section σDNCO(193 nm)=(2.6±0.2)×10−19 cm2 molecule−1 allowed the direct determination of the D atom product quantum yield of φD(193 nm)=(0.21±0.03). At the wavelength of 248 nm, where the optical absorption cross section was too small to be measured with reasonable accuracy, a kinetic calibration method was used to measure product quantum yields for D atom, φD(248 nm)=(0.77±0.10), and for "spin-forbidden" ND(X 3Σ−) formation, φND(248 nm)=(0.23±0.10). From the D atom Doppler profiles, measured under collision-free conditions, the fraction of the available energy released as product translational energy was determined to be fT(D+NCO)=(0.44±0.04) for 193 nm and fT(D+NCO)=(0.64±0.17) for 248 nm photolysis wavelengths. In addition, using polarized photodissociation laser light, measurements were carried out in order to determine the anisotropy of the D atom product angular distribution. It was found that the value of the anisotropy parameter β decreases from −(0.45±0.09) for a photolysis wavelength of 193 nm to −(0.01±0.10) at 248 nm, suggesting a moderately anisotropic distribution at the shorter wavelength and an effectively isotropic one at the longer wavelength. Comparisons are made with results from recent photodissociation dynamics studies of the isotopomer HNCO. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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