Experimental and numerical analysis of Tm2+ excited-states dynamics and luminescence in CaX2 (X = Cl, Br, I)

Journal Article (2021)
Authors

M. P. Plokker (TU Delft - RST/Luminescence Materials)

I.C. van der Knijff (TU Delft - Optical Technologies)

A.V. de Wit (Student TU Delft)

B. Voet (Student TU Delft)

T. Woudstra (Student TU Delft)

V. Khanin (TU Delft - RST/Luminescence Materials)

P. Dorenbos (TU Delft - RST/Luminescence Materials)

Erik van der Kolk (TU Delft - RST/Luminescence Materials)

Research Group
RST/Luminescence Materials
Copyright
© 2021 M.P. Plokker, I.C. van der Knijff, A.V. de Wit, B. Voet, T. Woudstra, V. Khanin, P. Dorenbos, E. van der Kolk
To reference this document use:
https://doi.org/10.1088/1361-648X/abfa5d
More Info
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Publication Year
2021
Language
English
Copyright
© 2021 M.P. Plokker, I.C. van der Knijff, A.V. de Wit, B. Voet, T. Woudstra, V. Khanin, P. Dorenbos, E. van der Kolk
Research Group
RST/Luminescence Materials
Issue number
25
Volume number
33
DOI:
https://doi.org/10.1088/1361-648X/abfa5d
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Abstract

The prospect of using Tm2+-doped halides for luminescence solar concentrators (LSCs) requires a thorough understanding of the temperature dependent Tm2+ excited states dynamics that determines the internal quantum efficiency (QE) and thereby the efficiency of the LSC. In this study we investigated the dynamics in CaX2:Tm2+ (X = Cl, Br, I) by temperature- and time-resolved measurements. At 20 K up to four distinct Tm2+ emissions can be observed. Most of these emissions undergo quenching via multi-phonon relaxation below 100 K. At higher temperatures, only the lowest energy 5d–4f emission and the 4f–4f emission remain. Fitting a numerical rate equation model to the data shows that the subsequent quenching of the 5d–4f emission is likely to occur initially via multi-phonon relaxation, whereas at higher temperatures additional quenching via interband crossing becomes thermally activated. At room temperature only the 4f–4f emission remains and the related QE becomes close to 30%. Possible reasons for the quantum efficiency not reaching 100% are provided.