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  • 1
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 714-726 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Photostimulated desorptions (PSD's) of CO, CO+, and CO− from a Pt surface are studied theoretically using Pt2–CO model cluster including image force correction. Calculations are performed by the single excitation configuration interaction and the symmetry adapted cluster (SAC)/SAC-CI methods. The PSD's of the ground state CO occur as the Menzel–Gomer–Redhead (MGR) process and those of CO+ (n cation) and excited (n→π*) CO* through the modified MGR process in which the upper repulsive potential curves are nonadiabatic; the process proceeds through a sequence of nonadiabatic transitions between the similar pertinent states embedded in the metal excited bands. The excited states as the desorption channels are characterized by the excitations from the Pt–CO bonding orbitals to the antibonding MO's: metal-adsorbate chemical bond cleavage by photons which leads to a repulsive potential is essential for the PSD. The electrostatic image force interaction plays only a minor role and the present result does not support the Antoniewicz model. The calculated excitation-energy thresholds for the CO, CO+, and CO* desorptions are 1.6∼2.6, 11.3, and 11.3–12.7 eV, respectively, which explains the energy thresholds and the fluence dependencies of the incident laser in the PSD experiments. On the other hand, the PSD giving CO− would occur with the energy range of 6.2–8.2 eV, one to two photon energy of the 193 nm (6.4 eV) laser. Since the upper nonadiabatic potential curves have shallow minima, in this case, the lifetime of the CO− species would be larger than those of the CO+ and CO* species. The present study clarifies the electronic structures of the desorbed CO+, CO−, and CO* species, which have not been identified experimentally. © 1996 American Institute of Physics.
    Materialart: Digitale Medien
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  • 2
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 103 (1995), S. 6993-6998 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The ground and excited states of Ni(CO)4 are studied using the symmetry adapted cluster (SAC)/SAC-configuration interaction (SAC-CI) method. The experimental absorption spectrum is well reproduced by the present calculations. All the peaks observed in the range of 200∼350 nm are assigned to the electronic allowed 1T2 excited states. The third peak is assigned to the 3 1T2 and 4 1T2 states. Next, the potential energy curves of the ground and the low-lying excited states are calculated by the same method and utilized to clarify the mechanism of the photofragmentation reaction of Ni(CO)4 by a XeCl laser (308 nm). A reaction pathway involving several excited states is proposed for the photofragmentation reaction into the excited Ni(CO)3 and CO. The calculated emission energy from the former agrees well with the observed luminescence spectrum. © 1995 American Institute of Physics.
    Materialart: Digitale Medien
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  • 3
    Digitale Medien
    Digitale Medien
    s.l. : American Chemical Society
    Organometallics 12 (1993), S. 3398-3404 
    ISSN: 1520-6041
    Quelle: ACS Legacy Archives
    Thema: Chemie und Pharmazie
    Materialart: Digitale Medien
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  • 4
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 83 (1985), S. 723-734 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The symmetry-adapted cluster (SAC) expansion and the SAC-CI theory have been applied to the calculations of the valence and Rydberg excitations and ionizations of the five-membered ring compounds, pyrrole, furan, and cyclopentadiene. For almost all cases, the experimental values were reproduced to within 0.3 eV for the excitation energy, and to within 0.5–0.7 eV for the ionization potential. We have given several new assignments for the excitation spectra of pyrrole and furan, and the first ab initio assignments for cyclopentadiene. However, there were remarkable disagreements of about 1.2 eV for the singlet π → π* excitations of 2 1A1 state for furan, and of 1 1B2 state for cyclopentadiene. This is the same tendency as those due to the MRSD-CI method. For ionization potential, our assignments of the peaks are essentially the same as those due to the Green's function method by von Niessen et al., but the present SAC-CI method reproduces the experimental data better than this method.
    Materialart: Digitale Medien
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  • 5
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 87 (1987), S. 1169-1182 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The SAC (symmetry-adapted cluster) expansion and the SAC-CI theory are applied to the calculations of the valence and Rydberg excitations and the ionizations of benzene. The active space consists of 80 MO's including both π and σ spaces; viz., 35π+45σ for the valence excitations and ionizations and 29π+51σ for the Rydberg excitations. For the lower six valence excited states, 3B1u(T1), 3E1u(T2), 1B2u(S1), 3B2u(T3), 1B1u(S2), and 1E1u(S3), generated from the π(e1g)→π*(e2u) transitions, the excitation energies are reproduced to within 0.5 eV of the experimental values with the average discrepancy being 0.34 eV. The first three states are explainable within the π electron space. For the other three states, the σ-reorganization effect is very important; viz., 0.6, 0.7, and 0.8 eV for the T3, S2, and S3 states, respectively. The polarizationdπ function also works to lower the T3 and S2 states by 0.3 and 0.4 eV, respectively. The total lowerings from the SDT π-CI of Hay and Shavitt to the 35π+45σ SAC-CI are about 1 eV for these three states. With including the σ-reorganization effect, the diffuse nature of the S3 state, a typical V state, decrease from 〈x2〉=62 (π SAC-CI) to 41 (π+σ SAC-CI) a.u., in comparison with the ground state value of 30 a.u. Accordingly, the oscillator strength changes from 0.61 (π SAC-CI) to 1.03 (π+σ SAC-CI). The first systematic theoretical study is given for the Rydberg excitations including both π and σ states. With the aid of the recent experimental studies due to the MPI (multiphoton ionization) spectroscopy, the lower Rydberg excited states are almost completely identified. The SAC-CI results agree with the experimental values to within 0.3 eV for all the Rydberg states studied here. The σ-reorganization effect on the Rydberg transitions is about 0.3 eV. The SAC-CI calculation further gives satisfactory results for the outer and inner valence ionizations and their satellite peaks. The theoretical ionization spectrum well reproduces the general trends of the observed ESCA spectrum.
    Materialart: Digitale Medien
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  • 6
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 114 (2001), S. 8990-8999 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The outer- and inner-valence ionization spectra of the Group VI hydrides H2O, H2S and H2Se below the double-ionization threshold were studied by the SAC-CI (symmetry-adapted-cluster configuration-interaction) general-R method. The SAC-CI method quite accurately reproduced the experimental spectra of these hydrides and gave detailed characterizations of the shake-up states. Several unknown satellite peaks were predicted. The shake-up state which includes excitations to the Rydberg orbitals was found to be very important for describing the satellite peaks of these hydrides. A detailed inner-valence satellite spectrum of H2Se is theoretically proposed prior to any experimental observation. © 2001 American Institute of Physics.
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  • 7
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 435-439 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Hyperfine splitting constants of the ground 2B1 and excited 2A1 states of NH2 radical are calculated by the symmetry adapted cluster-configuration interaction method with the use of the basis set which satisfies the cusp condition at the position of the nucleus. The calculated values compare well with the experimental values when the vibrational effects are considered for the 2A1 state. The nature of the vibrational wave functions for the double well 2A1 potential is discussed in some detail.
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  • 8
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 6205-6214 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: A method of calculating hyperfine splitting constants (hfsc) of open-shell radicals is reported. Since the hfsc reflects a very local property of the wave function at the position of the nuclei, we use Slater-type orbitals (STOs) which have cusps at the centers. Spin correlation (spin polarization) and electron correlation are taken into account with the use of the SAC-CI (symmetry adapted cluster-configuration interaction) theory. Configuration selection is not done since energy and spin density are very different properties. The dimensions of the matrices involved in the SAC-CI method are small enough to permit such a procedure. The integrals necessary for the SCF and SAC-CI methods are calculated by the STO-6G method with the use of the available Gaussian program, and the hfsc's and the cusp values are calculated from the original STOs. Several STOs are examined for H+2 and H2O+. The resultant standard method is applied to the organic π and σ radicals CH3, CH3CH2, CH3NH, CH3O, CH3OCH+3, H2CO+, CH2CH, and HCO. The present results of hfsc's show generally better agreement with experiment than the previous calculations based on the Gaussian-type orbitals (GTOs). In particular, the present results are free from the theoretical dilemma seen for the GTO calculations that a variationally better wave function does not necessarily give a better hfsc. This is important in developing a reliable theory for calculating hfsc's.
    Materialart: Digitale Medien
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  • 9
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 5759-5769 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Reactions of a hydrogen molecule with small platinum clusters Ptn (n=1,2,3) are studied theoretically by ab initio methods. This provides a cluster model study for hydrogen chemisorption on a Pt surface. The results suggest that the Pt atom and the linear Pt3 cluster will react with H2 and dissociatively adsorb it, making two Pt–H bonds, whereas the Pt2 cluster will not react with H2 because of a high energy barrier. The dissociative adsorption of a hydrogen molecule occurs at a side-on, on-top site of a surface Pt atom and molecular adsorption does not seem to occur. Essentially only one Pt atom is involved in the initial adsorption process. These findings are in contrast to the palladium case previously reported. Almost no energy barrier exists for the hydrogen migration from one Pt atom to an adjacent one, with a preference being shown for one H atom on each Pt atom rather than two H atoms on one Pt atom. The heat of adsorption, the stability of the catalytic surface, etc., are best represented by the Pt3–H2 system. Spin–orbit coupling effect is examined for the Pt–H2 system and found to be small for the singlet A1 state which is the most important state for the dissociative adsorption. This effect is important, however, to obtain natural potential curve in the large Pt–H2 separation.
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  • 10
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 4913-4925 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The SAC (symmetry-adapted cluster) and SAC-CI theories are applied to the calculations of the valence excitations and the ionizations of pyridine. The active space consists of 85 MOs (35π and 50 σ MOs). For the valence π→π* and n→π* excited states, S1(1 1B2), S2(1 1A1), S3(2 1B2), Sn(1 1B1), T1(1 3A1), and Tn(1 3B1), the calculated excitation energies are higher than the experimental values by within ∼0.7 eV. Although the S4(2 1A1) state is experimentally considered not to be split from S3, the present calculation predicted it to be higher than S3 by 0.31 eV. The average discrepancy from the experimental data is 0.55 eV without including S4. The transition energies and some other properties are predicted for the valence π→π* excited states, T2(1 3B2), T3(2 3A1), T4(2 3B2) and for the n→π* excited states, S'n(1 1A2) and Tn(1 3A2), for which the experimental values are unavailable so far. The following two observations seem to be interesting. (i) The valence π→π* excited states of pyridine are understood from those of benzene, reported previously, as a result of perturbation, an alteration of one C–H group to an isoelectronic nitrogen atom. The typical V states, S3 and S4, show large σ-reorganization effect, which is detected as the change in the transition energy and some one electron properties. (ii) For the relative positions between the π→π* and n→π* excitations, our results are as follows. The lowest singlet excited state is n→π*[Sn(1 1B2)]. The lowest triplet state isπ→π*[T1(1 3A1)] and n→π*[Tn(1 3B1)] exists higher than T1 by 0.15 eV. Experimentally, the lowest singlet excitation is confirmed to be n→π*, but two controversial assignments exist for the lowest triplet state: π→π* or n→π*. For the ionization potential, the experimental spectra is reproduced to within ∼0.6 eV. The nature of the first three peaks are calculated as nππ, which is supported by some recent experimental studies. The similarity and difference in the satellite peaks of benzene and pyridine are pointed out.
    Materialart: Digitale Medien
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