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Charge Carrier Trapping Processes in RE(2)O(2)S (RE = La, Gd, Y, and Lu)
[Image: see text] Two different charge carrier trapping processes have been investigated in RE(2)O(2)S:Ln(3+) (RE = La, Gd, Y, and Lu; Ln = Ce, Pr, and Tb) and RE(2)O(2)S:M (M = Ti(4+) and Eu(3+)). Cerium, praseodymium and terbium act as recombination centers and hole trapping centers while host int...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2017
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5413963/ https://www.ncbi.nlm.nih.gov/pubmed/28479942 http://dx.doi.org/10.1021/acs.jpcc.7b01577 |
Sumario: | [Image: see text] Two different charge carrier trapping processes have been investigated in RE(2)O(2)S:Ln(3+) (RE = La, Gd, Y, and Lu; Ln = Ce, Pr, and Tb) and RE(2)O(2)S:M (M = Ti(4+) and Eu(3+)). Cerium, praseodymium and terbium act as recombination centers and hole trapping centers while host intrinsic defects provide the electron trap. The captured electrons released from the intrinsic defects recombine at Ce(4+), Pr(4+), or Tb(4+) via the conduction band. On the other hand, Ti(4+) and Eu(3+) act as recombination centers and electron trapping centers while host intrinsic defects act as hole trapping centers. For these codopants we find evidence that recombination is by means of hole release instead of electron release. The released holes recombine with the trapped electrons on Ti(3+) or Eu(2+) and yield broad Ti(4+) yellow-red charge transfer (CT) emission or characteristic Eu(3+) 4f–4f emission. We will conclude that the afterglow in Y(2)O(2)S:Ti(4+), Eu(3+) is due to hole release instead of more common electron release. |
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