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Description
| - 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)
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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)
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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)
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skos:notation
| - RIV/60076658:12520/12:43883653!RIV13-MSM-12520___
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http://linked.open...avai/riv/aktivita
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http://linked.open...avai/riv/aktivity
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http://linked.open...iv/cisloPeriodika
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http://linked.open...vai/riv/dodaniDat
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http://linked.open...aciTvurceVysledku
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http://linked.open.../riv/druhVysledku
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http://linked.open...iv/duvernostUdaju
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http://linked.open...titaPredkladatele
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http://linked.open...dnocenehoVysledku
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http://linked.open...ai/riv/idVysledku
| - RIV/60076658:12520/12:43883653
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http://linked.open...riv/jazykVysledku
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http://linked.open.../riv/klicovaSlova
| - CR; ELECTRON-GAS; CRYSTAL-STRUCTURE (en)
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http://linked.open.../riv/klicoveSlovo
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http://linked.open...odStatuVydavatele
| - US - Spojené státy americké
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http://linked.open...ontrolniKodProRIV
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http://linked.open...i/riv/nazevZdroje
| - JOURNAL OF MATERIALS SCIENCE
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http://linked.open...in/vavai/riv/obor
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http://linked.open...ichTvurcuVysledku
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http://linked.open...cetTvurcuVysledku
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http://linked.open...vavai/riv/projekt
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http://linked.open...UplatneniVysledku
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http://linked.open...v/svazekPeriodika
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http://linked.open...iv/tvurceVysledku
| - Reshak, Ali Hussain
- Auluck, S.
- Kamarudin, H.
- Chen, Xuean
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http://linked.open...ain/vavai/riv/wos
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issn
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number of pages
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http://bibframe.org/vocab/doi
| - 10.1007/s10853-012-6476-1
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http://localhost/t...ganizacniJednotka
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