330 research outputs found

    Photoionization of tungsten ions: experiment and theory for W4+^{4+}

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    Experimental and theoretical results are reported for single-photon single ionization of the tungsten ion W4+^{4+}. Absolute cross sections have been measured employing the photon-ion merged-beams setup at the Advanced Light Source in Berkeley. Detailed photon-energy scans were performed at 200~meV bandwidth in the 40 -- 105~eV range. Theoretical results have been obtained from a Dirac-Coulomb R-matrix approach employing basis sets of 730 levels for the photoionization of W4+^{4+}. Calculations were carried out for the 4f145s25p65d2  3FJ4f^{14}5s^2 5p^6 5d^2 \; {^3}{\rm F}_{J}, JJ=2, ground level and the associated fine-structure levels with JJ=3 and 4 for the W4+^{4+} ions. In addition, cross sections have been calculated for the metastable levels 4f145s25p65d2  3P0,1,2,1D2,1G4,1S04f^{14}5s^2 5p^6 5d^2 \; {^3}{\rm P}_{0,1,2},{^1}{\rm D}_{2},{^1}{\rm G}_{4},{^1}{\rm S}_{0}. Very satisfying agreement of theory and experiment is found for the photoionization cross section of W4+^{4+} which is remarkable given the complexity of the electronic structure of tungsten ions in low charge states.Comment: 15 pages, 3 figures, to appear in the Journal of Physics B: Atomic, Molecular and Optical Physic

    Single-photon single ionization of W+^{+} ions: experiment and theory

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    Experimental and theoretical results are reported for photoionization of Ta-like (W+^{+}) tungsten ions. Absolute cross sections were measured in the energy range 16 to 245 eV employing the photon-ion merged-beam setup at the Advanced Light Source in Berkeley. Detailed photon-energy scans at 100 meV bandwidth were performed in the 16 to 108 eV range. In addition, the cross section was scanned at 50 meV resolution in regions where fine resonance structures could be observed. Theoretical results were obtained from a Dirac-Coulomb R-matrix approach. Photoionization cross section calculations were performed for singly ionized atomic tungsten ions in their 5s25p65d4(5D)6s  6DJ5s^2 5p^6 5d^4({^5}D)6s \; {^6}{\rm D}_{J}, JJ=1/2, ground level and the associated excited metastable levels with JJ=3/2, 5/2, 7/2 and 9/2. Since the ion beams used in the experiments must be expected to contain long-lived excited states also from excited configurations, additional cross-section calculations were performed for the second-lowest term, 5d^5 \; ^6{\rm S}_{J}, JJ=5/2, and for the 4^4F term, 5d^3 6s^2 \; ^4{\rm F}_{J}, with JJ = 3/2, 5/2, 7/2 and 9/2. Given the complexity of the electronic structure of W+^+ the calculations reproduce the main features of the experimental cross section quite well.Comment: 23 pages, 7 figures, 1 table: Accepted for publication in J. Phys. B: At. Mol. & Opt. Phy

    The structure of Cu(110) (2×3)–N; pseudo‐square reconstruction of a rectangular mesh substrate

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    The structure of the Cu(110)(2×3)–N phase has been investigated by parallel studies using 3‐keV Li+ and 2‐keV He+ion scattering and scanned energy mode normal emission N 1s photoelectron diffraction. The Li+ion scattering results provide clear evidence for anadsorbate‐induced reconstruction of the Cu surface and, in particular, indicate a shortening of the Cu–Cu atomic spacing along the 〈100〉 azimuth to a value of 2.7±0.1 Å, similar to the 〈110〉 spacing of 2.55 Å. A model of the surface consistent with this result involves a pseudo‐square Cu top atom layer with N atoms occupying alternate hollow sites leading to a local structure which is a 6% distorted Cu(100)c(2×2)–N phase. He+ion scattering data provides support for the N hollow adsorption sites. Scanned energy mode photoelectron diffraction is insensitive to the nature of the reconstruction but provides information on the local adsorption sites and, hence, on the lateral registry of the reconstructed overlayer and the underlying substrate
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