Charge Carrier Trapping Processes in RE2O2S (RE = La, Gd, Y, and Lu)

Journal Article (2017)
Author(s)

Hongde Luo (TU Delft - RST/Fundamental Aspects of Materials and Energy)

Adrie J.J. Bos (TU Delft - RST/Fundamental Aspects of Materials and Energy)

Pieter Dorenbos (TU Delft - RST/Fundamental Aspects of Materials and Energy)

Research Group
RST/Fundamental Aspects of Materials and Energy
Copyright
© 2017 H. Luo, A.J.J. bos, P. Dorenbos
DOI related publication
https://doi.org/10.1021/acs.jpcc.7b01577
More Info
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Publication Year
2017
Language
English
Copyright
© 2017 H. Luo, A.J.J. bos, P. Dorenbos
Research Group
RST/Fundamental Aspects of Materials and Energy
Issue number
16
Volume number
121
Pages (from-to)
8760-8769
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Abstract

Two different charge carrier trapping processes have been investigated in RE2O2S:Ln3+ (RE = La, Gd, Y, and Lu; Ln = Ce, Pr, and Tb) and RE2O2S:M (M = Ti4+ and Eu3+). 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 Ce4+, Pr4+, or Tb4+ via the conduction band. On the other hand, Ti4+ and Eu3+ 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 Ti3+ or Eu2+ and yield broad Ti4+ yellow-red charge transfer (CT) emission or characteristic Eu3+ 4f–4f emission. We will conclude that the afterglow in Y2O2S:Ti4+, Eu3+ is due to hole release instead of more common electron release.