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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
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 103 (1995), S. 1303-1308 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Spectra of fluoromethylene radicals, HCF and DCF, have been observed between 304 and 325 nm using mass-resolved, resonance enhanced multiphoton ionization (REMPI). Singlet HCF is generated by sequential reactions of atomic fluorine in either methane or methyl fluoride. The spectra arise from two-photon resonances between the ground state X˜ 1A′ and the previously unobserved E˜ 1A′ (3p) Rydberg state. The band origins lie at T0=62154±2 cm−1 (321.69±0.01 nm) and T0=62175±2 cm−1 (321.58±0.01 nm) (2σ) above the ground states for HCF and DCF, respectively. Vibrational resolution and partial rotational resolution are obtained, with ν2′=1128±4 cm−1 and ν3′=1614±4 cm−1 for HCF and ν1′=2095±5 cm−1, ν2′=872±3 cm−1, and ν3′=1582±4 cm−1 for DCF (2σ). Under typical experimental conditions, the strongest peak for HCF is due to the 210310 resonance at 308.23±0.04 nm and the strongest peak for DCF is due to the 220 resonance at 312.85±0.01 nm. The results of vibrational and rotational analyses are consistent with predictions from ab initio calculations, which also yield the adiabatic ionization potential IPa=10.06±0.05 eV (2σ).
    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 100 (1994), S. 3422-3428 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We report resonance enhanced multiphoton ionization (REMPI) spectra of gas-phase indium monochloride (InCl) between 330 and 490 nm. The spectra originate from one-, two-, and three-photon resonances with electronic states that reside between 27 000 and 75 000 cm−1. We assign 12 new Rydberg states. From these Rydberg origins we can extrapolate the adiabatic ionization potential IPa=77 460±600 cm−1 (9.60±0.08 eV). The Rydberg states exhibit vibrational frequencies ranging between 307 and 355 cm−1.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 68 (1997), S. 2978-2989 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A miniature-cavity realization of the cavity ring-down concept, which permits extension of the technique to spectroscopy of surfaces, thin films, liquids, and, potentially, solids, is explored using a wave-optics model. The novel spectrometer design incorporates a monolithic, total-internal-reflection-ring cavity of regular polygonal geometry with at least one convex facet to induce stability. Evanescent waves generated by total-internal reflection probe absorption by matter in the vicinity of the cavity. Optical radiation enters or exits the resonator by photon tunneling, which permits precise control of input and output coupling. The broadband nature of total-internal reflection circumvents the narrow bandwidth restriction imposed by dielectric mirrors in conventional gas-phase cavity ring-down spectroscopy. Following a general discussion of design criteria, calculations are presented for square and octagonal cavity geometries that quantify intrinsic losses and reveal an optimal cavity size for each geometry. Calculated absorption spectra for the NO3 radical from 450 to 750 nm in a nitric acid solution are presented to demonstrate bandwidth and sensitivity.
    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 87 (1987), S. 4546-4558 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The reactions of F(2P)+ketene and F(2P)+ketene-d2 were studied in a flow reactor. Spectra of the radical products CH2F, CD2F, CH, CF, and atomic carbon were detected between 292–395 nm by resonance enhanced multiphoton ionization (REMPI) mass spectrometry. Fluoromethyl radicals were identified as a major product of the F+ketene elementary reaction. REMPI spectra of fluoromethyl radicals originated from two-photon preparation of 3p, 4p, and 5p Rydberg states (quantum defect ∼0.6). Absorption of a third laser photon ionized the radicals, a 2+1 REMPI mechanism. Rydberg band origins were observed in CH2F at ν00=52 863, 63 275, and 67 265 cm−1 and in CD2F at ν00=52 786, 63 195, and 67 186 cm−1. A normal mode analysis revealed the vibrational frequencies of the C–F stretch, CH2 scissors, and out-of-plane bending modes in the Rydberg states. The ground state out-of-plane bending frequency in CH2F is 260(30) cm−1 and in CD2F it is 170(30) cm−1. CH radicals were generated by the photolysis of ketene and observed at ∼311 nm by two-photon excitation through the D 2Π(v′=2) ←←X 2Πr band. The reaction mechanism that generated the CF radicals was not determined. The REMPI CF radical spectrum generated by a 2+1 photon mechanism appeared as a series of bandheads described by the constants ν00=∼52 572 cm−1, ωe =1820 cm−1, and ωexe =−18.2 cm−1.
    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 84 (1986), S. 5262-5270 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The resonance enhanced multiphoton ionization (REMPI) spectra of CH2OH, CH2OD, CD2OH, and CD2OD between 420–495 nm are reported. Analysis of the excited state vibrational band progressions shows that the spectrum originates from simultaneous two photon absorption to form a 3p Rydberg state (ν00=40 064 cm−1) of the radical. Absorption of a third photon ionized the radical. A normal mode analysis of the REMPI spectra enabled assignments of six active vibrational modes in the excited state. The no isomerization of methoxy radicals into hydroxymethyl radicals was observed. The experimental measurement uncertainty limits this isomerization rate to less than 2.9 s−1 at 300 K.
    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 87 (1987), S. 1977-1981 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The resonance enhanced multiphoton ionization (REMPI) spectrum of O2 a 1Δg between 305 and 350 nm is reported. The spectrum is compared to the REMPI spectrum of ground state molecular oxygen in the same electronic energy region, and a number of differences in the respective spectra are observed. Detection limits for O2 a 1Δg by REMPI is calculated to be 5×109 molecule cm−3 in the ion source of the mass spectrometer.
    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 82 (1985), S. 4426-4433 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We report the resonance enhanced multiphoton ionization spectra of ClO and BrO free radicals between 415 and 475 nm. The observed electronic states were prepared by simultaneous absorption of three identical photons from a dye laser. Absorption of at least one additional photon induced ionization. ClO showed spectra originating from the D, E, and F states previously reported by N. Basco and R. D. Morse. The origin of the F 2Σ←X 2Πi bands were reassigned to ν00=70 183 cm−1 and ν00=69 868 cm−1. BrO showed three new vibrational progressions originating from transitions between the X 2Π3/2 state to Rydberg states with assignments of E 2Σ (ν00=65 003 cm−1), F 2Σ (ν00=67 470 cm−1), and an apparently inverted state, designated G (ν00=70 504 cm−1), that possesses orbital angular momentum greater than zero. The G-state bands were separated by 139(±3) cm−1 which should approximate the magnitude of the spin-orbit coupling constant of this excited state if it is of 2Πi symmetry.
    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 99 (1993), S. 7521-7528 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: AlCl was detected and characterized with 1+2, 2+1, 2+2, 3+1, and 3+2 resonance-enhanced multiphoton ionization spectroscopy using laser light between 332 and 570 nm. AlCl was generated in the gas phase with high temperature reaction of Al with InCl3, or by the reaction of Al with AgCl. New states residing between 52 000 and 66 000 cm−1 were identified. Vibrational intervals of the new Rydberg states are about 20% greater than those of AlCl (X 1Σ+), with most lying between 565–595 cm−1.
    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 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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