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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. 7690-7699 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The adsorption and desorption kinetics for Xe on three Pt single crystalline surfaces have been measured using threshold temperature programmed desorption measurements. It has been found that the first-order desorption kinetic parameters at zero coverage for Xe on Pt(111) (E0d =5.73±0.50 kcal/mol; ν0d=1012.5±0.9 s−1) are in excellent agreement with measurements made by a modulated molecular beam method [E0d =5.65±0.35 kcal/mol; ν0d=1012.1 s−1]. The presence of step defect sites of varying density on Pt(557) (1/6 defects) and on Pt(112) (1/3 defects) is shown to have a marked influence on Xe desorption kinetics, producing larger values of E0d(approximately-equal-to)8.5–8.7 kcal/mol and larger values of ν0d (approximately-equal-to)1014 s−1 compared to Pt(111). In addition, for Pt(111), slight attractive Xe–Xe interactions are observed, whereas for Xe adsorption on step sites, repulsive Xe–Xe interactions are observed as the steps fill. Xe adsorption kinetics on Pt(111) at 87 K are consistent with an island growth mechanism. In contrast, on Pt(557) and Pt(112), the adsorption process does not seem to produce island growth on the terraces. These results, taken together, show that using Xe, defect sites on metals may be probed effectively with adsorption and desorption kinetic methods.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 7700-7707 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: NO photodesorption from the oxygen-covered, oxidized, and sulfur-saturated Ni(111) surfaces was studied. Temperature programmed desorption effectively discriminates between NO species adsorbed on Ni metal sites and on Ni sites modified by O or S, making the study of photodesorption from each site possible. Oxygen- and sulfur-modified Ni(111) surfaces both exhibit enhanced photodesorption cross sections compared to a clean Ni surface. Both the direct observation of NO(g) photodesorption and postirradiation thermal desorption measurements of NO coverage have been carried out. The photodesorption process is first order in photon flux and in NO coverage within a given chemisorption state. The photon-energy dependence of the NO photodesorption cross section from oxidized and S-saturated Ni(111) surfaces was measured in detail over a photon energy range of 1.5–3.8 eV. For both oxidized and sulfur-saturated Ni(111), the threshold for NO photodesorption is ∼1.5 eV. In addition, the photodesorption cross sections are dependent on the adsorption states of NO on the modified Ni(111) surfaces. The mechanisms of NO photodesorption are discussed and it is proposed that NO photodesorption is probably induced by the valence electron excitation from the occupied NO 2π*-d state to the unoccupied NO 2π*-d state. However, a hot electron model originating from the substrate cannot be excluded. The quenching of electronically excited NO on the clean Ni(111) surface is efficient.
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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. 5700-5711 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The kinetics of the thermal recombinative desorption of hydrogen from the monohydride phase on the Si(100) surface has been studied by laser-induced thermal desorption (LITD). A rate law that is first order in the atomic hydrogen coverage with an activation energy of 45 kcal/mol gives an accurate fit to the data over a temperature range of 685–790 K and a coverage range of 0.006 to 1.0 monolayer. A new mechanism is proposed to explain these surprising results, namely, that the rate limiting step of the reaction is the promotion of a hydrogen atom from a localized bonding site to a delocalized band state. The delocalized atom then reacts with a localized atom to produce molecular hydrogen which desorbs. Evidence to support these conclusions comes from isotopic mixing experiments. Studies of recombinative desorption from other surfaces of silicon, which had been assumed to obey second-order kinetics, are discussed in the light of these results.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 4320-4326 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photon-induced desorption studies of chemisorbed CO on Ni(111), Ni(111) with chemisorbed oxygen, and oxidized Ni(111) surfaces have been carried out. Only the oxidized Ni(111) surface exhibits measurable CO photodesorption in the energy range from 1.8 to 4.1 eV. Both direct observation of CO photodesorption and post-irradiation thermal desorption of CO have been performed. The photodesorption process is first order in photon flux and in CO coverage. At a photon energy of 4.1 eV, the cross section for CO photodesorption is measured to be 5×10−18 cm2. The measured threshold energy, 2.7±0.5 eV, is in good agreement with a model involving the O2−2p→Ni2+3d interband transition in NiO as the excitation process leading to photodesorption.
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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. 2208-2213 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Both NO and CO preferentially chemisorb on step sites of the Pt(112) crystal orienting the intermolecular bond in the downstairs direction. Using the digital electron stimulated desorption-ion angular distribution method (ESDIAD), an elliptical angular distribution of the desorbing O+ ions was detected from the NO/Pt(112) system, with the longer axis of the ellipse normal to the step-edge direction. On the other hand, the O+ ESDIAD pattern from the CO/Pt(112) system shows an approximately cylindrical symmetric shape. Heating of the crystal leads to broadening of the ion desorption patterns in both cases without change in the patterns' elliptical or circular cross-sectional geometry. These results are interpreted as being due to ion desorption from NO molecules bonded to two Pt atoms on the step edge and vibrating with a longer amplitude in the direction perpendicular to the step. In the case of CO, bonded to a single Pt atom, the amplitude of vibration is approximately the same in directions parallel and perpendicular to the step edge. Thus, in certain cases ESDIAD patterns may be used to determine the hybridization state of adsorbates.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 8798-8807 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Ab initio molecular electronic structure theory has been used in conjunction with flexible basis sets to predict the barrier height to radical dissociation for the lowest triplet state (T1) of formaldehyde (3A‘H2CO→H⋅+HCO⋅). Self-consistent-field (SCF), complete active space SCF (CASSCF), and configuration interaction with single and double excitations (CISD) levels of theory were employed with basis sets ranging from double zeta plus polarization (DZP) to quadruple zeta plus triple polarization (QZ3P). Complete geometry optimizations of the equilibrium structure of X˜ 1A1 H2CO, a˜ 3A‘H2CO, the transition state, and the dissociated radical on the potential energy surface were carried out. Improved basis set, triple zeta plus double polarization with higher angular momentum polarization functions [TZ(2df,2pd)], single point methods were used to further refine relative energies. Higher correlated level, multireference CISD (MR-CISD), was employed to verify the calculations involving higher excitations. At the highest level of theory [CISD(Q) with the TZ(2df,2pd) basis set], the exit barrier height at 0 K for the T1 state is predicted to be 7.8 kcal mol−1 with the zero point vibrational energy (ZPVE) correction with an estimated error bar of 3.0 kcal mol−1, favorably comparing with the most recent and accurate experimental estimate of 2.9–6.0 kcal mol−1 by Chuang, Foltz, and Moore [J. Chem. Phys. 87, 3855 (1987)]. This study also presents the most sophisticated theoretical predictions to date on the equilibrium structure and physical properties of the lowest triplet state, a˜ 3A‘, of formaldehyde.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 8105-8109 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Jackels and Davidson's interpretation of the symmetry-breaking problem in the NO2 radical is examined using complete active space self-consistent-field (CASSCF) wave functions. Jackels and Davidson provided a Lewis-structure analysis of the necessary forms of C2v -restricted wave functions for 2B2 NO2. In particular, C2v and single-configuration restrictions force the molecule to "choose'' between the beneficial effects of resonance and the adverse effects of inclusion of charged components in the wave function. This choice, according to Jackels and Davidson, results in a distortion to Cs symmetry in the region of the 2B2 minimum. The Cs symmetry complete active space treatment enables NO2 to achieve wave functions of proper symmetry (for both 2A1 and 2B2 states, when C2v nuclear symmetry is present) while simultaneously yielding significantly localized orbitals, thus offering a means to verify the earlier analysis. Although the Cs complete active space results contradict one important Jackels–Davidson result by predicting a very shallow C2v 2B2 energy minimum for NO2, the authors find the earlier molecular orbital picture of NO2 to be a useful tool for qualitatively understanding its electronic structure.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 7085-7093 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Electro-optical absorption measurements have been made on four model nitroaromatics to determine the effect of twisting of the donor–acceptor single bond on the charge-transfer characteristics in the Franck–Condon excited states. Observed ground- and excited-state dipole moments of nitromesitylene, which has been treated experimentally as the nonplanar analogue of planar nitrobenzene, indicate that electronic excitation of twisted nitrobenzene results in a nearly full unit charge transfer from donor (benzene) to the acceptor (nitro) group (Δμ=18.3 D). On the other hand, in planar nitrobenzene and nitronaphthalene the charge transfer is more delocalized over the whole molecular skeleton, resulting in normal changes in dipole moment (Δμ=5–10 D). In the analogous anthracene system, i.e., 9-nitroanthracene, the charge transfer upon electronic excitation is extremely low (Δμ=1.7 D), which is reflected by its very small change in the dipole moment. Therefore, it is evident that the charge-transfer processes in the twisted molecules are quite different for different aromatic ring systems. Simple molecular-orbital calculations satisfactorily explain the reason for such differences on the basis of their highest occupied molecular-orbital (HOMO) and lowest unoccupied molecular-orbital (LUMO) characteristics. Transition moment directions have also been obtained experimentally and compared with the theoretically predicted directions based on the symmetry properties of the HOMO and LUMO. Agreement is found in all cases studied.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 5119-5126 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present experimental and calculated vibration–rotation spectra as a function of temperature for the methoxy species (–OCH3 and –OCD3) chemisorbed on an alumina surface. The axis of rotation is the C–O bond axis. The model for our calculations is that of free rotation, and we describe the methods employed here in full detail. The qualitative agreement between the calculated and experimental spectra suggests that the adsorbed methoxy species is undergoing free rotational motion about the C–O bond axis.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 4459-4466 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Ab initio molecular orbital theory has been used to investigate the barrier to inversion in NF+(overdot)3. Complete geometry optimizations have been carried out with a variety of basis sets and electron correlation methods. It is shown that for this problem the use of single-point energy calculations needs to be treated with caution. Discrepancies amongst previous theoretical values are shown to be due to the use of inappropriate geometries and inadequate inclusion of electron correlation. With a variety of quantum chemical methods, the barrier to inversion is predicted to be in the range 11.3–13.3 kcal/mol. We have also predicted the vibrational splittings for the NF+(overdot)3 potential energy surface and attempted to reconcile the differences with experiment.
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