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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. 530-538 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: NH4+(NH3)n (n=0–3) cluster ions are produced in a field-free flow tube section of a selected ion flow–drift tube (SIFDT) apparatus. Cluster ion mobilities are measured in mixtures of He and NH3 and used to obtain the individual mobilities in helium and in ammonia by applying Blanc's law to the mixtures. Mobilities of the cluster ions are also measured in pure helium by producing the ions in the ion source of a flowing afterglow, selected ion flow–drift tube apparatus (FA-SIFDT). The measurements in pure helium compare well with the mobilities in helium obtained by applying Blanc's law to the mixtures. The zero field mobilities of the cluster ions in helium are 22.1±0.4 cm2 V−1 s−1 for NH4+, 16.6±0.4 cm2 V−1 s−1 for NH4+(NH3), 12.2±0.4 cm2 V−1 s−1 for NH4+(NH3)2, and 12.1±0.4 cm2 V−1 s−1 for NH4+(NH3)3. The decrease with increasing size of the cluster can be explained in terms of the sizes of the geometric cross sections. The zero-field mobilities in NH3 are 0.94±0.35 cm2 V−1 s−1 for NH4+, 0.83±0.22 cm2 V−1 s−1 for NH4+(NH3), 0.50±0.27 cm2 V−1 s−1 for NH4+(NH3)2, and 0.25±0.20 cm2 V−1 s−1 for NH4+(NH3)3. The small values of the mobilities in these polar gas systems are understood in terms of the strong ion–dipole interactions. Calculated mobilities in NH3 are obtained by computing the collision cross section with the ion–dipole interactions taken into account; the results compare well with the measurements for NH4+ and NH4+(NH3). However, the measured mobilities of the larger cluster ions are smaller than the computed values. The discrepancies may be due to several factors including dipole–dipole interactions, ligand exchange reactions, formation of long-lived quasibound complexes, and efficient transfer of kinetic energy into internal energy of the cluster ion and the ammonia molecules. © 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 112 (2000), S. 10269-10281 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotational state-resolved velocity component distribution functions of N2+ (ν″=0) drifted in helium are measured in a flow-drift apparatus by the technique of single-frequency laser-induced fluorescence (LIF). A single-mode ring dye laser is used to probe Doppler profiles of various rotational lines in the R-branch of the (ν′,ν″)=(0,0) band of the B 2Σu+–X 2Σg+ system at 390 nm, with the laser propagation direction set either parallel or perpendicular to the drift field. A small but definite (3%) increase in ion mobility with increasing rotational state from J=13.5 to J=22.5 is observed at a fixed field strength of 12 Td. Mobilities of J=15.5 measured over the range of 1.5–16 Td yield a K0(0) of 22.0 cm2 V−1 s−1 and are in good agreement with earlier arrival-time measurements. Parallel translational temperatures are found to be significantly higher than perpendicular temperatures; a difference of at least 140 K between these temperatures is measured for J=15.5 at 16 Td. No discernible difference between the parallel translational temperatures for different rotational states is observed. There is evidence for a small degree of positive skewness (third central moment) in the parallel velocity component distributions, the first observation of such an effect in a molecular ion-atomic buffer system. Previous results that indicated poor agreement between CO+–He pulsed-field arrival-time and LIF mobilities are discussed; the LIF results were most likely hampered by space-charge effects. © 2000 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 105 (1996), S. 5455-5466 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The charge transfer reaction of N+2(v=0–4)+Kr→N2+Kr+ is studied at thermal energy as a function of vibrational excitation in the reactant ion. The selected-ion flow tube technique coupled with laser-induced fluorescence detection is used to measure the vibrationally state specific rate constants. A dramatic vibrational enhancement is observed; measured rate constants are 1.0 (±0.6)×10−12, 2.8 (±0.3)×10−12, 2.1 (±0.2)×10−11, 5.1 (±0.2)×10−11, and 8.3 (±0.4)×10−11 cm3 molecule−1 s−1 for v=0, 1, 2, 3 and 4, respectively. Mass spectrometric kinetics experiments are also performed to confirm that vibrational relaxation, N+2(v)+Kr→N+2(v′〈v)+Kr, is a negligible process. The charge transfer for v=0 is extremely slow in spite of the large exothermicity (e.g., 0.915 eV for the production of N2(v′=0)+Kr+(2P1/2) states), yet the reaction is enhanced when the apparent energy mismatch is greater for the vibrationally excited reactant. A simple model is proposed to explain the experimental results at thermal energies ((very-much-less-than)1 eV). The model assumes that only the most energy-resonant exothermic transitions, N+2(v)+Kr→N2(v+3)+Kr+(2P1/2), occur within the duration of the ion–molecule collision complex and that the charge transfer takes place with probabilities governed by the corresponding Franck–Condon factors. However, the Franck–Condon factors are modified by a trial displacement of 0.02 A(ring) to account for the changes in vibrational wave functions of N+2 and N2 during a close approach of the (N2–Kr)+ pair; this method gives an excellent description of the experimental results. © 1996 American Institute of Physics.
    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 64 (1993), S. 2808-2820 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A selected ion flow tube apparatus is coupled with laser induced fluorescence (LIF) detection for the selective monitoring of ion vibrational states and their reactions. Mass selected ions are injected into a flow tube with a venturi inlet using He carrier gas. A 200 Hz dye laser system provides sensitive LIF detection of the injected ions at densities as low as 1×105 cm−3 for N+2. The rotational temperatures of the N+2 ions are estimated to be ≈300 K using the LIF detection, while the vibrational temperatures can be high and may be varied by the injection potentials. Vibrationally state-selected ion-molecule reactions of N+2(v=0, 1, and 2) are studied with N2, Ar, and O2 at thermal kinetic energies (Elab〈0.1 eV), where translation-to-vibration energy transfer is negligible. Isotopically specific charge-transfer reactions of 15N+2(v) with 14N2 are also studied. The ability to mass select ions and characterize their vibrational states and those of their reaction products allows novel studies of state-to-state ion chemistry.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Accounts of chemical research 14 (1981), S. 146-153 
    ISSN: 1520-4898
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    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 87 (1987), S. 5578-5579 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: First results are presented on velocity distribution measurements of Ba+ ions drifted in helium using a well-characterized drift tube and single-frequency laser-induced fluorescence detection. Reduced mobilities of Ba+ in helium are obtained for E/N values between 7.74 and 23.2 Td. The velocity distributions that are observed parallel to the electric field fit a displaced Maxwell–Boltzmann distribution, in agreement with theoretical predictions. However, the temperatures parallel and perpendicular to the field are not in good agreement with theoretical treatments.
    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 83 (1985), S. 601-610 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The nascent vibrational state distribution of the N++CO→CO+(v=0–2)+N charge transfer reaction is measured at thermal energy. The reaction is carried out in a flowing afterglow and the vibrational state populations are determined by laser-induced fluorescence on the CO+(A 2Π−X 2Σ+) system. The nascent vibrational state distribution for the N++ CO reaction is (0.71±0.05)v=0:(0.27±0.04)v=1:(0.02±0.01)v=2. The observed vibrational distribution suggests that neither a long-range Franck–Condon mechanism nor an energy resonant process adequately describes the charge transfer reaction. A dual channel mechanism of the reaction is considered, in which a fraction of the reactive collisions proceed by a long-range Franck–Condon mechanism while the remainder proceed via a long-lived NCO+ intermediate. The intermediate may lead to the observed extent of CO+ vibrational excitation either through statistical partitioning of the energy or by dynamical changes in the CO bond length through specific molecular orbital occupancies.
    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 114 (2001), S. 6654-6661 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Experimental results are presented for the rotational alignment of N2+(v″=0) as a function of both rotational state and component Doppler velocity. A single-frequency ring dye laser is used to probe the alignment of N2+ drifted in helium in a flow-drift apparatus by the technique of polarized laser-induced fluorescence. The collision-induced quadrupole rotational alignment parameter A0(2) is determined as a function of the field direction component of sub-Doppler laboratory velocity at a fixed field strength of 12 Td for five rotational states. A dramatic difference in velocity-selected alignment as a function of rotational state is observed, with the higher rotational states exhibiting a greater degree of alignment than the lower rotational states. Additionally, for sufficiently low rotational state (J=11.5), A0(2) changes sign across the Doppler profile, a behavior that has not previously been reported in the literature. A companion theoretical paper presents molecular dynamics calculations that are in excellent agreement with these experimental observations. © 2001 American Institute of Physics.
    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 84 (1986), S. 2158-2166 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Absolute branching ratios for production of O(3P), O(1D), and O(1S) in the reaction of N+ with O2 are measured using the flowing afterglow/visible chemiluminescence technique. The O(1S) product is monitored by the O(1S)–O(1D) emission at 557.7 nm. The O(1D) product is monitored via sensitized fluorescence at 760 nm from O2(b 1Σ+g) formed by energy transfer from O(1D) to O2(X 3Σ−g). Absolute O(1D) and O(1S) yields of 70±30% and ≤0.1%, respectively, of the total atomic oxygen product are inferred by comparison to the known O(1S) and O2(1Σ+g) emission intensities from the reaction of Ar(3P) with O2. The low O(1S) yield is also obtained directly from the relative O(1S) and O2(1Σ+g) emission intensities from the title reaction. A qualitative reaction mechanism consistent with these observations is presented.
    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 83 (1985), S. 3913-3918 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Product vibrational state distributions for the ion–molecule reactions F−+HBr,DBr→HF(v≤4), DF (v≤6)+Br− are determined using the flowing afterglow infrared chemiluminescence technique. The nascent distributions are (0.09±0.04)v=1@B: (0.29±0.04)v=2@B: (0.34±0.04)v=3@B: (0.28±0.04)v=4 for the HF product, and (0.05±0.04)v=1@B: (0.12±0.04)v=2@B: (0.16±0.04)v=3@B: (0.25±0.04)v=4@B: (0.22±0.04)v=5@B: (0.20±0.04)v=6 for the DF product. The fractions of the available energy deposited in product vibration are 0.60±0.04 and 0.63±0.05 for the proton transfer and deuteron transfer reactions, respectively. A surprisal analysis suggests that less than 5% of the product molecules are formed in v=0. The HF distribution is somewhat hotter than that reported previously, while the DF distribution is measured for the first time. Both distributions are remarkably similar to those reported for the analogous neutral processes, which suggests that direct collisions dominate the reactive encounters despite the presence of a deep attractive well in the potential surface for the ion–molecule reactions.
    Type of Medium: Electronic Resource
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