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Photon management with lanthanides
Efficient conversion of photons from high energy radiation (e.g. ultraviolet or X-rays) to lower energies (visible) has been optimized by using luminescent materials based on the optical properties of lanthanide ions. Presently, luminescent materials with efficiencies close to the theoretical maximu...
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Published in: | Optical materials 2006-05, Vol.28 (6), p.575-581 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Efficient conversion of photons from high energy radiation (e.g. ultraviolet or X-rays) to lower energies (visible) has been optimized by using luminescent materials based on the optical properties of lanthanide ions. Presently, luminescent materials with efficiencies close to the theoretical maximum are applied in e.g. fluorescent tubes, X-ray imaging and color television. Contrary to the mature status of luminescent materials in these fields, areas requiring new luminescent materials are emerging. There is great challenge in research on up- and downconversion materials and lanthanide ions are the prime candidates to achieve efficient materials. Here downconversion processes will be discussed for VUV phosphors with Pr
3+. The efficiency of resonant energy transfer of the
1S
0–
1I
6 energy from Pr
3+ to Eu
3+and Mn
2+ is investigated. The aim is to convert the 405
nm photon of the first step of the well-known cascade emission of Pr
3+ into a more useful visible photon. For co-doping with Eu
3+ it is observed that the Pr
3+ emission is quenched, most probably through a metal-to-metal charge-transfer state. The energy transfer from Pr
3+ to Mn
2+ is found to be inefficient.
An alternative for downconversion through resonant energy transfer is the non-resonant process of cooperative sensitization. For the Tb–Yb couple efficient cooperative energy transfer from the
5D
4 level of Tb
3+ to two Yb
3+ neighbors is observed with a transfer rate of 0.26
ms
−1. This corresponds to an upper limit of 188% for the conversion efficiency of visible (490
nm) photons to infrared (∼1000
nm) photons. |
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ISSN: | 0925-3467 1873-1252 |
DOI: | 10.1016/j.optmat.2005.09.055 |