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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 485-488 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The electronic spectrum of the AsF2 radical was observed between 330 and 380 nm using one-color, mass-resolved, 2+1 resonance enhanced multiphoton ionization (REMPI) spectroscopy. The spectrum arises from two-photon resonances with the F˜ (T0=54 355±15 cm−1, ν1′=813±6 cm−1, and ν2′=308±5 cm−1) and H˜ (T0=57 480±15 cm−1, ν1′=810±10 cm−1, and ν2′=310±20 cm−1), Rydberg states. A third photon ionized the radicals. The REMPI spectrum exhibits vibrational hot bands that give spectroscopic constants for AsF2 (X˜ 2B1) of ν1″=705±10 cm−1 and ν2″=285±10 cm−1. Solutions of the Rydberg equation indicate that plausible assignments for the F˜ and H˜ states are limited to the set of 4d and 5p Rydberg states.© 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 58 (1991), S. 2309-2311 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on the production of atomic hydrogen subsequent to the 193 nm photolysis of triethylarsenic (TEAs) using an excimer laser. The H atoms are probed via two-photon (121.6+364.7 nm) ionization, and the resulting H atom Doppler profile at Lyman-α is presented. Photolysis power dependence studies demonstrate that substantial H atom formation occurs at relatively low laser powers. However, the H atom signal actually begins to diminish as the photolysis laser power is increased beyond ∼70 MW/cm2. Correlations with time-of-fight mass spectral data suggest that ion channels are being accessed. The possible mechanisms for TEAs excitation that lead to H atom formation/depletion are presented, and the implications of these observations on controlling carbon incorporation in the laser-enhanced growth of films of GaAs, AlGaAs, etc. are 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 98 (1993), S. 3732-3736 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The 3p 2B1←←X˜ 2B1 bands of CH2D and CHD2 radicals were observed between 305 and 335 nm by mass resolved, 2+1 resonance enhanced multiphoton ionization spectroscopy. Spectroscopic constants were found for the 3p 2B1 Rydberg state of the CH2D radical (ν00=59 940 cm−1, ν1a1 CH2 stretch=2995 cm−1, ν2a1 CD stretch=2220 cm−1, ν4b1 out-of-plane large amplitude (OPLA)=1260 cm−1, ν5b2 CH2 asymmetric stretch=3055 cm−1, ν6b2 CD bend=1115 cm−1) and of the CHD2 radical (ν00=59 920 cm−1, ν1a1 CH stretch=3040 cm−1, ν2a1 CD2 stretch=2150 cm−1, ν4b1 OPLA=1165 cm−1, ν6b2 CH bend=1210 cm−1). Vibrational frequencies calculated by ab initio theory agree well with the experimental data.
    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 93 (1990), S. 7946-7950 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A rate-equation approach is presented that models H-atom formation during the pulsed laser photolysis of a triethyl metal compound, the specific case being triethylaluminum excited at 193 nm. An excimer laser initiates the chemistry under collisionless conditions, and H atoms are produced that are detected using two-photon (121.6+364.7 nm) ionization. Experimentally, the H-atom intensity is monitored as a function of photolysis laser power. Mechanistically, the primary photodissociation step is postulated to involve cleavage of the metal–carbon bond, thereby producing an ethyl radical. This species can then either: (1) form C2H4 and H directly; or (2) absorb an additional photon and produce an H-atom photofragment. The rate equations and their solutions allow one to calculate how H-atom production should vary as a function of photolysis laser power, and the interplay between the two H-atom production channels is calculated for various absorption cross sections and dissociation rates. A comparison with experimental power dependence data suggests that an overall one-photon dissociation process predominates under the experimental conditions actually used.
    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 93 (1990), S. 7504-7505 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Results are reported on the 193 and 248 nm photolysis of iodoethane, specifically with respect to H-atom production. Experiments using selectively deuterated iodoethanes, ICD2CH3 and ICH2CD3, reveal that at 193 nm the carbon–hydrogen bond cleavage is not carbon-atom specific. However, following photolysis at 248 nm, it is clear that C–H (or C–D) bond dissociation occurs preferentially at the β carbon atom.
    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 95 (1991), S. 2200-2202 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Experiments involving two photolysis lasers and one probe laser demonstrate that 248 nm excimer laser radiation will induce C–H bond cleavage preferentially at the β position in the ethyl radical. To facilitate carbon site labeling, selectively deuterated chloroethanes (ClCH2CD3 and ClCD2CH3) are used as precursor compounds. Two-photon ionization via resonance with the Lyman-α transition is used to detect H (or D) atoms. An initial 193 nm photolysis pulse serves to cleave the C–Cl bond in ClCH2CH3, while a second pulse at 248 nm dramatically enhances H-atom production. Experiments on ClCH2CD3 and ClCD2CH3 clearly show that this enhancement occurs preferentially through carbon–hydrogen bond cleavage at the β carbon site. It is apparent that 248 nm photon absorption by the ethyl radical is an important step in the overall mechanism.
    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 98 (1993), S. 1178-1192 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Selectively deuterated compounds are used to investigate the "site-specific'' nature of H-atom production resulting from the photolysis of primary haloalkanes. The molecules investigated are 1-iodopropane, 1-bromopropane, iodoethane, bromoethane, and chloroethane, with photolysis being initiated at 193, 222, and 248 nm. Hydrogen and deuterium isotopes are systematically used to label chemically distinct carbon atoms within a given molecule. H- and D-atom Doppler profiles are generated via two-photon (121.6+364.7 nm) ionization resonant with Lyman-α, and the relative H/D ratios are used to quantify the probability for hydrogen production from each carbon site. In general, photolysis of an intermediate, presumably the alkyl radical, is implicated as being a key step in the overall process. When using 248 nm radiation, the photolysis process is dominated by C–H (or C–D) bond cleavage at the β carbon position regardless of the system investigated. In contrast, results using 193 nm excitation display no obvious preference for bond cleavage at a particular carbon site, again regardless of the system. The data produced by 222 nm photolysis show a qualitative tendency for C–H (or C–D) bond cleavage at the β carbon, but the quantitative results are not as self-consistent as either the 248 nm or the 193 nm data. Also, the results of ab initio calculations on the ground and excited states of the ethyl radical are used to help interpret the observed site specificity.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 56 (1990), S. 695-697 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Results are reported on the 193 nm excitation of trimethylaluminum under collisionless conditions. Time-of-flight mass spectra are monitored at several different excimer laser powers. At relatively low powers, the mass spectra consist solely of masses 27 and 57, presumably the Al+ and Al(CH3)+2 ions. At higher laser powers, however, mass 58 is readily observed, suggesting the presence of a reaction channel involving α-hydrogen elimination to form the AlH(CH3)2 photofragment. This observation is interpreted in the context of recent theoretical calculations by Higashi and Steigerwald [Appl. Phys. Lett. 54, 81 (1989)].
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 113 (1991), S. 1432-1434 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 95 (1991), S. 8676-8680 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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