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DC Field | Value | Language |
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dc.contributor.author | den Engelsen, D | - |
dc.contributor.author | Fern, GR | - |
dc.contributor.author | Ireland, TG | - |
dc.contributor.author | Silver, J | - |
dc.date.accessioned | 2018-01-15T16:58:26Z | - |
dc.date.available | 2018-01-15T16:58:26Z | - |
dc.date.issued | 2018-01-02 | - |
dc.identifier.citation | den Engelsen, D., Fern, G.R., Ireland, T.G. and Silver, J. (2018) 'Cathodoluminescence of Y2O3:Ln3+ (Ln ¼ Tb, Er and Tm) and Y2O3:Bi3+ nanocrystalline particles at 200 keV', RSC Advances, 2018, 8 (1), pp. 396 - 405 (10). doi: 10.1039/c7ra12644a. | en_US |
dc.identifier.uri | https://bura.brunel.ac.uk/handle/2438/15666 | - |
dc.description.abstract | Copyright © 2018 The Author(s). The cathodoluminescence (CL) spectra of nanocrystalline Y2O3:Tb3+ (0.3%), Y2O3:Er3+ (1%), Y2O3:Tm3+ (2%) and Y2O3:Bi3+ (1%) were recorded in a transmission electron microscope at 200 keV, low current density and various temperatures. The quenching energy of the intrinsic luminescence of the various Y2O3:Ln3+ (Ln = Tb, Er and Tm) phosphors was found to be 0.25 eV. The intrinsic luminescence and the strongest spectral transitions of Ln3+ in these three phosphors exhibit similar temperature behaviour at temperatures > −50 °C, viz. a small increase of the spectral radiance upon increasing the temperature. Increasing the temperature beyond −50 °C led to complete quenching of the intrinsic luminescence at room temperature, whereas the radiance of the Ln3+ spectral transitions only decreased slightly. An extended Jablonski diagram for the energy transfer from the self-trapped exciton states in Y2O3 to the Ln3+ and Bi3+ ions is proposed. This diagram also indicates why Tb3+ is a better quencher of the intrinsic luminescence in Y2O3 than Er3+ and Tm3+. The intrinsic luminescence of Y2O3:Bi3+ largely overlapped with the blue Bi3+ emission band, which made an accurate analysis of its temperature behaviour impossible. Nevertheless, we concluded that upon increasing the temperature energy from Bi3+ ions at the C3i sites is transferred to Bi3+ ions at C2 sites. From the temperature behaviour of the 539 nm transition of the 2H11/2 → 4I15/2 manifold of Y2O3:Er3+ the activation energy for this transition could be determined: viz. 0.078 eV (623 cm−1). | en_US |
dc.description.sponsorship | Engineering and Physical Sciences Research Council and Technology Strategy Board (TSB) PURPOSE (TP11/MFE/6/1/AA129F; EP-SRC TS/G000271/1) and CONVERTED (JeS no. TS/1003053/1), PRISM (EP/N508974/1) and FAB3D programs. TSB CONVERT program. | en_US |
dc.format.extent | 396 - 405 (10) | - |
dc.format.medium | Electronic | - |
dc.language.iso | en | en_US |
dc.publisher | The Royal Society of Chemistry | en_US |
dc.rights | Copyright © 2018 The Author(s). Open Access Article. Published on 02 January 2018. This article is licensed under a Creative Commons Attribution 3.0 Unported Licence (https://creativecommons.org/licenses/by/3.0/). | - |
dc.rights.uri | https://creativecommons.org/licenses/by/3.0/ | - |
dc.subject | Cathodoluminescence | en_US |
dc.title | Cathodoluminescence of Y2O3:Ln3+ (Ln ¼ Tb, Er and Tm) and Y2O3:Bi3+ nanocrystalline particles at 200 keV | en_US |
dc.type | Article | en_US |
dc.identifier.doi | https://doi.org/10.1039/c7ra12644a | - |
dc.relation.isPartOf | RSC Advances | - |
pubs.issue | 1 | - |
pubs.publication-status | Published | - |
pubs.volume | 8 | - |
dc.identifier.eissn | 2046-2069 | - |
dc.rights.holder | The Author(s) | - |
Appears in Collections: | Wolfson Centre for Sustainable Materials Development and Processing Dept of Mechanical and Aerospace Engineering Research Papers |
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