2015
DOI: 10.1007/978-90-481-2879-2_3
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High Energy Spectroscopy and Resonance Effects

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Cited by 2 publications
(4 citation statements)
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“…Figure presents XANES and XEOL spectra measured for the oleylamine-capped La 1– x – y Tb x Eu y OCl nanocrystals. In Figure A, the XANES spectra show element-specific (4d → 4f) forbidden 1 S 0 → 3 D 1 and allowed 1 S 0 → 3 P 1 absorptions characteristic of trivalent lanthanum at 101.7 and 117.5 eV, respectively, similar to spectra observed in Figure A for nanocrystals grown using TOPO as the passivating ligand. ,, The XEOL spectra acquired using X-ray excitation at the center of the giant resonance (at 117.5 eV) are plotted in Figure B; spectra acquired for the multiply doped solid-solution nanocrystals are contrasted with spectra measured for La 0.941 Eu 0.059 OCl and La 0.911 Tb 0.089 OCl nanocrystals under the same conditions. Intriguingly, the characteristic 5 D 4 → 7 F J green emission and 5 D 3 → 7 F J blue emission bands of Tb 3+ are dominant for all of the multiply alloyed samples, even for materials where the ratio of divalent europium atoms to trivalent terbium atoms approaches 4:1.…”
Section: Resultssupporting
confidence: 54%
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“…Figure presents XANES and XEOL spectra measured for the oleylamine-capped La 1– x – y Tb x Eu y OCl nanocrystals. In Figure A, the XANES spectra show element-specific (4d → 4f) forbidden 1 S 0 → 3 D 1 and allowed 1 S 0 → 3 P 1 absorptions characteristic of trivalent lanthanum at 101.7 and 117.5 eV, respectively, similar to spectra observed in Figure A for nanocrystals grown using TOPO as the passivating ligand. ,, The XEOL spectra acquired using X-ray excitation at the center of the giant resonance (at 117.5 eV) are plotted in Figure B; spectra acquired for the multiply doped solid-solution nanocrystals are contrasted with spectra measured for La 0.941 Eu 0.059 OCl and La 0.911 Tb 0.089 OCl nanocrystals under the same conditions. Intriguingly, the characteristic 5 D 4 → 7 F J green emission and 5 D 3 → 7 F J blue emission bands of Tb 3+ are dominant for all of the multiply alloyed samples, even for materials where the ratio of divalent europium atoms to trivalent terbium atoms approaches 4:1.…”
Section: Resultssupporting
confidence: 54%
“…117.5 eV (this feature is about 10 eV above the ionization threshold, reflecting strong electron correlation in these systems) . The broad line shape of this absorption feature is indicative of a short lifetime . Given the relatively low concentrations of Eu 3+ and Tb 3+ , absorption features corresponding to the giant resonances of the luminescent centers are not observed in the XANES spectra.…”
Section: Resultsmentioning
confidence: 96%
“…Interestingly, the 1 S 0 → 3 D 1 transition observed in the pre-edge region is forbidden by LS selection rules but is nevertheless observed as a result of strong spinorbit coupling. 53 Because of the low concentration of Eu 3+ and Eu 2+ in the matrix, no discernible giant resonance feature is observed for these species.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…10 eV above the ionization threshold, which reflects the strong electron correlation of the 4f electrons localized within a narrow band (this effect is further amplified in later lanthanides). The pronounced enhancement of the absorption cross-section of the 1 S 0 → 1 P 1 giant resonance and its broad line shape indicate a much shorter lifetime of the excitation as compared to the excitation to the triplet final state. Interestingly, the 1 S 0 → 3 D 1 transition observed in the pre-edge region is forbidden by LS selection rules but is nevertheless observed as a result of strong spinorbit coupling . Because of the low concentration of Eu 3+ and Eu 2+ in the matrix, no discernible giant resonance feature is observed for these species.…”
Section: Resultsmentioning
confidence: 99%