208 research outputs found

    R-matrix calculation of electron collisions with electronically excited O2 molecules

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    Low-energy electron collisions with O2_2 molecules are studied using the fixed-bond R-matrix method. In addition to the O2_2 X3Σg−{X}^3\Sigma_{g}^- ground state, integrated cross sections are calculated for elecron collisions with the a1Δg{a}^1\Delta_{g} and b1Σg+{b}^1\Sigma_{g}^+ excited states of O2_2 molecules. 13 target electronic states of O2_2 are included in the model within a valence configuration interaction representations of the target states. Elastic cross sections for the a1Δg{a}^1\Delta_{g} and b1Σg+{b}^1\Sigma_{g}^+ excited states are similar to the cross sections for the X3Σg−{X}^3\Sigma_{g}^- ground state. As in case of excitation from the X3Σg−{X}^3\Sigma_{g}^- state, the O2−_2^- Πu\Pi_u resonance makes the dominant contribution to excitation cross sections from the a1Δg{a}^1\Delta_{g} and b1Σg+{b}^1\Sigma_{g}^+ states. The magnitude of excitation cross sections from the a1Δg{a}^1\Delta_{g} state to the b1Σg+{b}^1\Sigma_{g}^+ state is about 10 time larger than the corresponding cross sections from the X3Σg−{X}^3\Sigma_{g}^- to the b1Σg+{b}^1\Sigma_{g}^+ state. For this a1Δg{a}^1\Delta_{g} →\to b1Σg+{b}^1\Sigma_{g}^+ transition, our cross section at 4.5 eV agrees well with the available experimental value. These results should be important for models of plasma discharge chemistry which often requires cross sections between the excited electronic states of O2_2.Comment: 26 pages, 10 figure

    Electron attachment to valence-excited CO

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    The possibility of electron attachment to the valence 3Π^{3}\Pi state of CO is examined using an {\it ab initio} bound-state multireference configuration interaction approach. The resulting resonance has 4Σ−^{4}\Sigma^{-} symmetry; the higher vibrational levels of this resonance state coincide with, or are nearly coincident with, levels of the parent a3Πa^{3}\Pi state. Collisional relaxation to the lowest vibrational levels in hot plasma situations might yield the possibility of a long-lived CO−^- state.Comment: Revtex file + postscript file for one figur

    Convergence of CI single center calculations of positron-atom interactions

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    The Configuration Interaction (CI) method using orbitals centered on the nucleus has recently been applied to calculate the interactions of positrons interacting with atoms. Computational investigations of the convergence properties of binding energy, phase shift and annihilation rate with respect to the maximum angular momentum of the orbital basis for the e^+Cu and PsH bound states, and the e^+-H scattering system were completed. The annihilation rates converge very slowly with angular momentum, and moreover the convergence with radial basis dimension appears to be slower for high angular momentum. A number of methods of completing the partial wave sum are compared, an approach based on a Delta X_J = a/(J + 1/2)^n + b/(J + 1/2)^(n+1) form (with n = 4 for phase shift (or energy) and n = 2 for the annihilation rate) seems to be preferred on considerations of utility and underlying physical justification.Comment: 23 pages preprint RevTeX, 11 figures, submitted to PR

    The Dipole Moment of Styrene

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    The dipole moment of styrene, calculated from eighteen solutions ranging in weight fraction from 0 - 100%, was found to be 0.181 D. The method and results of the measurement were compared to the method and results of Petro and Smyth for the same compound. It was concluded that the atomic polarization in styrene in small, and thus is taken into account by the measurement of the molar refraction at the sodium D line. It was further proposed that the relatively large dipole moments of trans-p, βdinitrostyrene and trans-p, βdicyano-styrene may be due, at least in part, to abnormally large atomic polarizations

    The Dipole Moments and Molar Refractions of Several Trans-Beta-Nitrostyrenes

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    The dipole moments and molar refractions are reported for p-nitrostyrene (4.24 D, 44.3 ml.), trans-betanitrostyrene (4.50 D, 45.7 ml.), the p-methoxy (5.45 D, 56.3 ml.), p-methyl (4.97 D, 52.0 ml.), p-fluoro (3-12 D, 45.5ml), p-chloro (2.90 D, 51.8 ml.), p-bromo (3.02 D, 54.4 ml.), p-iodo (3.26 D, 58.0 ml.), p-nitro (0.83 D, 52.0 ml.), and p-cyano 0.96 D, 47.9 ml.) derivatives of trans-beta-nitrostyrene. It is suggested that the large dipole moments obtained for the p-nitro and p-cyano-beta-nitrostyrenes may be due to unusually large atomic polarizations which would not be taken into consideration by the present method of measurement and calculation

    Towards the electron EDM search: Theoretical study of HfF+

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    We report first ab initio relativistic correlation calculations of potential curves for ten low-lying electronic states, effective electric field on the electron and hyperfine constants for the ^3\Delta_1 state of cation of a heavy transition metal fluoride, HfF^+, that is suggested to be used as the working state in experiments to search for the electric dipole moment of the electron. It is shown that HfF^+ has deeply bound ^1\Sigma^+ ground state, its dissociation energy is D_e=6.4 eV. The ^3\Delta_1 state is obtained to be the relatively long-lived first excited state lying about 0.2 eV higher. The calculated effective electric field E_eff=W_d|\Omega| acting on an electron in this state is 5.84*10^{24}Hz/(e*cm)Comment: 4 page
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