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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 7135-7155 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Infrared double resonance spectroscopy has been used to study state-resolved rotational and vibrational energy transfer in vibrationally excited SiH4. Completely specified rotational levels (v,J,Cn) are populated by CO2 laser radiation. Subsequent energy transfer is followed by diode laser transient absorption. The total relaxation efficiencies of the initially populated levels for self-collisions and collisions with Ar and CH4 follow the ordering σ(F2)〉σ(A2)〉σ(E) and are slightly larger than the Lennard-Jones cross sections. State-to-state rotational energy transfer in the ν4 vibration of SiH4 is extremely state specific. In addition to a differentiation between the A, E, and F symmetry levels, there is a selectivity with respect to the fine-structure levels within each rotational state. A preference for transfer to other levels of the same Coriolis sublevel of ν4 was found. This can be phrased as a Δ(J−R)=0 propensity rule. Principal pathways, only one per J per symmetry, are identified. Within each rotational level, the principal-pathway final states are closely spaced; this effect is related to the clustering of the rovibrational levels of the dyad. Large changes in J are possible in a single collision between silane molecules. A kinetic master equation has been used to model energy flow among rotational levels in silane, from which state-to-state energy transfer parameters could be extracted. Collision-assisted absorption of two CO2 photons into the triad has also been detected. A simple modification of the kinetic analysis allows us to obtain an estimate for the relaxation rate out of the triad levels. These laser pumping and relaxation processes determine the efficiency with which high vibrational levels of silane may be populated by infrared multiple photon excitation.
    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 90 (1989), S. 5434-5442 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Vibration–vibration (V–V) and vibration–translation (V–T) energy transfer efficiencies have been measured for the v4=1 mode of silane in collisions with He, Ar, Kr, H2, CH4, and itself, using the time-resolved infrared double-resonance technique. The V–V cross sections are approximately one-third to one-half of the Lennard-Jones cross sections, and show a variation with the nuclear–spin symmetry state (A, E, or F) of the molecule. The ν4 V–T deactivation efficiencies are in the range 0.0001–0.002, with the polyatomic molecules being about an order of magnitude more efficient than the noble-gas atoms. This can be quantitatively interpreted by the vibration–rotation (V–R) resonance transfer model of Poulsen et al. [J. Chem. Phys. 58, 3381 (1973)]. A simple breathing-sphere model does not, however, provide a good representation of the V–T collision efficiencies for rare gas–silane collisions.
    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 92 (1990), S. 4768-4777 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A definitive measurement of the rate coefficient for the quenching of N(2D) by O(3P) is reported. The O(3P) atoms were generated by titrating NO directly into the active nitrogen flow. Analysis of the results required that the rate coefficient for the reaction N(2D)+NO→N2+O be known accurately, and this was also determined. A finite mixing time correction is also necessary. The best estimate of the rate coefficient from this work is (6.9+0.7, −1.1)×10−13 cm3 s−1 at T=298 K, considerably smaller than a previous measurement [J. Phys. Chem. 92, 5977 (1988)] and in much better accord with values required by atmospheric models.
    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 88 (1988), S. 2027-2032 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have investigated the interaction of CF3 free radicals, produced by infrared multiple-photon dissociation of C2F6, with Si(100) and SiO2 surfaces. The CF3 radicals initially undergo dissociative chemisorption on the Si surface to produce surface carbides and fluorosilyl species. At higher coverages, the fluorine transfer reaction is inhibited. Significantly smaller amounts of the CF3 radical chemisorb on the oxide surfaces and those that do adsorb do not dissociate. Sputtering the oxide surface by argon ion bombardment increases the amount of radicals that can be adsorbed. Ion bombardment of the fluorocarbon overlayer on both surfaces results primarily in removal of the CF3 groups. The radical reactions cannot by themselves account for SiO2/Si selectivity in plasma reactive etching, but do appear to play an important role in anisotropic etching.
    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 92 (1990), S. 5164-5165 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotational relaxation times in ozone–ozone collisions have been measured for selected rovibrational levels using the time-resolved infrared double-resonance technique. Rotationally inelastic processes account for at least 90% of the measured pressure-broadening rate. The rotational-state dependence of the relaxation cross sections is in good accord with the collision models used in current theories of pressure broadening. The V–V energy transfer rate between symmetric and asymmetric stretching modes of ozone has also been measured; the V–V cross section is approximately 15 A(ring)2, about an order of magnitude smaller than that for rotational energy transfer.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 6742-6746 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Time-resolved infrared double resonance experiments have been carried out on silane. A pulsed CO2 laser is used to pump dyad←ground state transitions, and triad←dyad transitions are probed with a tunable diode laser. Two-photon (triad←ground state) signals are observed with the CO2 10P(20), 10P(22), and 10P(28) pump lines. Rotational relaxation rates have been measured for E, F2, and A2 symmetry components of the v4=1, J=13 level of silane in collisions with silane, argon, and methane. The relaxation efficiencies follow the order σrot (F2)〉σrot (A2)〉σrot (E), which parallels the behavior of pressure-broadening coefficients for infrared absorption lines of methane.
    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 86 (1987), S. 5909-5917 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have measured fluorescence lifetimes of individual rovibronic levels in SiH2 (A˜ 1B1, 020). The lifetimes vary widely from one level to the next, ranging from (approximately-less-than)10 ns to 〉1 μs. Similar behavior is seen in the (000), (010), and (030) levels. This behavior is interpreted in terms of coupling of the A˜ 1B1 rovibronic levels with background levels in the X˜ 1A1 (S0) and a˜ 3B1 (T1) states, and thence via predissociation to Si(3P)+H2. The irregular variation in the lifetimes reflects the quasirandom spacings of S0 and T1 levels in the vicinity of any particular A˜ state level.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 6838-6852 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An infrared double resonance laser spectroscopic technique is used to study state-resolved rotational and vibrational energy transfer in the isotopically substituted methane molecule,13CD4 . Molecules are prepared in a selected rovibrational state by CO2 laser pumping, with the quantum numbers v, J, and Cn completely specified. Measurements of both the total rate of depopulation by collisions, and the rates of transfer into specific final rovibrational states (v', J', Cn' ) are carried out using time-resolved tunable diode laser absorption spectroscopy. The depopulation rates due to collisions between methane and the rare gases are on the order of the Lennard-Jones collision frequencies. Self-relaxation is slightly more efficient than the Lennard-Jones estimate. The rather small relaxation rates are characteristic of a short-range potential, or "strong-collision'' regime, expected for a molecule without a dipole moment. The state-to-state energy transfer measurements reveal a dramatic selectivity of rotational energy transfer pathways with respect to the fine-structure rotational states Cn . Relaxation occurs through a surprisingly small subset of the energetically accessible pathways. Also suggested is a preference for population transfer to occur within the initial vibrational angular momentum sublevel of the ν4 (F2 ) vibrational state, which has three sublevels in consequence of Coriolis interaction. This preference can be formulated as a propensity for Δ(R−J)=0 transitions. We deduce that large changes of J(ΔJ∼5) can occur in single collisions between methane molecules, based on a simple kinetic model of the data. This is also characteristic ofshort-range collisions in which it is likely that no single multipolar interaction dominates. Collisional relaxation between the ν4 and ν2 bending vibrations proceeds more slowly than rotational relaxation, but as fast as transfer among the closely grouped stretching and bend-overtone levels, measured previously in CH4 . No evidence for rotationally specific V–V transfer is found. We discuss an exhaustive spectroscopic analysis of 13CD4 that provides unambiguous spectral assignments for use in detecting vibrationally excited molecules (v4 =1) in specific rotational states.
    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 86 (1987), S. 6561-6563 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Measured fluorescence lifetimes of individual rovibronic levels in SiH2 (A˜ 1B1, 0n0, n=1,2,3), vary irregularly from one level to the next. The distribution of these fluctuations is well fitted by the procedure of maximal entropy. This suggests that the intramolecular evolution at that energy range (∼18 000 cm−1) is chaotic and uniformly samples its available phase space.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 4476-4476 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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