About: Linear optical susceptibilities of the oxoborate (Pb3O)(2)(BO3)(2)WO4: theory and experiment     Goto   Sponge   NotDistinct   Permalink

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  • The optical susceptibilities have been investigated experimentally and theoretically for a newly synthesized oxoborate, (Pb3O)(2)(BO3)(2)WO4. The crystal structure is composed of one-dimensional chains formed by corner-sharing OPb4 tetrahedra. BO3 and WO4 groups are located around the chains to hold them together via Pb-O bonds. The solid-state fluorescence spectrum exhibited a maximum emission peak at around 375.2 nm with excitation light of 280 nm. UV-Vis diffuse reflectance spectra showed a band gap of about 2.9 eV which compares well with our theoretical band gap of about 2.3 eV obtained using the local density approximation and 2.6 eV using the Engel-Vosko's generalized gradient approximation. We have optimized the atomic positions starting from our X-ray diffraction data so as to minimize the forces on each atom. A remarkable finding is that this crystal possesses a weak anisotropy among three components of the frequency-dependent dielectric function and a small positive birefringence. This indicates that the oxoborate, (Pb3O)(2)(BO3)(2)WO4, cannot be used to produce second harmonic generation (SHG) and optical parametric oscillation.
  • The optical susceptibilities have been investigated experimentally and theoretically for a newly synthesized oxoborate, (Pb3O)(2)(BO3)(2)WO4. The crystal structure is composed of one-dimensional chains formed by corner-sharing OPb4 tetrahedra. BO3 and WO4 groups are located around the chains to hold them together via Pb-O bonds. The solid-state fluorescence spectrum exhibited a maximum emission peak at around 375.2 nm with excitation light of 280 nm. UV-Vis diffuse reflectance spectra showed a band gap of about 2.9 eV which compares well with our theoretical band gap of about 2.3 eV obtained using the local density approximation and 2.6 eV using the Engel-Vosko's generalized gradient approximation. We have optimized the atomic positions starting from our X-ray diffraction data so as to minimize the forces on each atom. A remarkable finding is that this crystal possesses a weak anisotropy among three components of the frequency-dependent dielectric function and a small positive birefringence. This indicates that the oxoborate, (Pb3O)(2)(BO3)(2)WO4, cannot be used to produce second harmonic generation (SHG) and optical parametric oscillation. (en)
Title
  • Linear optical susceptibilities of the oxoborate (Pb3O)(2)(BO3)(2)WO4: theory and experiment
  • Linear optical susceptibilities of the oxoborate (Pb3O)(2)(BO3)(2)WO4: theory and experiment (en)
skos:prefLabel
  • Linear optical susceptibilities of the oxoborate (Pb3O)(2)(BO3)(2)WO4: theory and experiment
  • Linear optical susceptibilities of the oxoborate (Pb3O)(2)(BO3)(2)WO4: theory and experiment (en)
skos:notation
  • RIV/60076658:12520/12:43883653!RIV13-MSM-12520___
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  • P(ED2.1.00/01.0024)
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  • 15
http://linked.open...vai/riv/dodaniDat
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  • Reshak, Ali Hussain
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  • 147120
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  • RIV/60076658:12520/12:43883653
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  • CR; ELECTRON-GAS; CRYSTAL-STRUCTURE (en)
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  • JOURNAL OF MATERIALS SCIENCE
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  • 47
http://linked.open...iv/tvurceVysledku
  • Reshak, Ali Hussain
  • Auluck, S.
  • Kamarudin, H.
  • Chen, Xuean
http://linked.open...ain/vavai/riv/wos
  • 000304110400022
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  • 0022-2461
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http://bibframe.org/vocab/doi
  • 10.1007/s10853-012-6476-1
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  • 12520
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