Hostname: page-component-76fb5796d-skm99 Total loading time: 0 Render date: 2024-04-26T07:25:32.745Z Has data issue: false hasContentIssue false

Thulium Doped Phosphors Under VUV Excitation

Published online by Cambridge University Press:  01 February 2011

Bernard Moine
Affiliation:
moine@pcml.univ-lyon1.fr, LPCML, Villeurbanne, France
Léna Beauzamy
Affiliation:
beauzamy@gmail.fr, LPCML, Villeurbanne, France
Richard S. Meltzer
Affiliation:
rmeltzer@physast.uga.edu, University od Georgia, Department of Physics and Astronomy, Athens, Georgia, United States
Get access

Abstract

Development of highly efficient mercury free fluorescent lamps and plasma display panels has been a challenging task due to the need for a combination of phosphor properties that are difficult to obtain in a single material (high efficiency, short emission lifetime and weak sensitivity to aging process under VUV excitation). Quantum cutting mechanism is a way to improve the fluorescence efficacy. Here we describe quantum cutting involving pairs of Tm3+ ions in KY3F10. Efficient excitation in the vacuum UV is initiated to the 5d state of Tm3+. This is followed by a cross relaxation energy transfer (CRET) involving the excited ion in the 5d state and nearby Tm3+ in the ground state, producing a pair of Tm3+ in excited states of the 4f13 configuration. Both ions can then emit photons. The excitation and reflection spectra are studied as a function of Tm3+ concentration and temperature. An unusual enhancement of the reflectivity at excitation wavelengths corresponding to the Tm3+ 5d absorption peaks is shown to arise from strong 5d→4f emission which is confirmed from the VUV emission spectra. The strong reduction of the integrated 5d emission intensity and shortening of its lifetime with Tm3+ concentration indicates the effective presence of the desired CRET process that is required for the first step of the quantum cutting. High Tm3+ concentrations are required for efficient quantum cutting. Whereas the CRET from the 5d state is estimated to be quite efficient, the 4f13 states of Tm3+ also undergo a strong CRET and therefore, emission from the 4f13 excited states that are created from the first step are strongly quenched at high Tm3+ concentrations. As a result, quantum yields greater than unity are not achieved.

Type
Research Article
Copyright
Copyright © Materials Research Society 2009

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Dieke, G. H., Spectra and Energy Levels of Rare Earth Ions in Crystals Interscience, New York, 1968.Google Scholar
2. Wegh, R. T., Meijerink, A., Lamminmaki, R. J., and Holsa, J., J. Lumin. 87–89, 1002 2000 Google Scholar
3. Dorenbos, P., J. Lumin. 91, 155 2000.Google Scholar
4. Moine, B., Bizarri, G., Varrel, B., Rivoire, J.Y., Optical Materials 29, 1148 (2007)Google Scholar
5. Makhov, V. N., Khaidukov, N. M., Lo, D., Krupa, J. C., Kirm, M., and Negodin, E., Optical Materials 27, 1131 (2005).Google Scholar
6. Wegh, R. and Meijerink, A. A., Phys Rev. B 60, 10820 (1999).Google Scholar