Abstract
The theory on the intensities of 4f→4f transitions introduced by B.R. Judd and G.S. Ofelt in 1962 has become a centerpiece in rare-earth optical spectroscopy over the past five decades. Many fundamental studies have since explored the physical origins of the Judd-Ofelt theory and have proposed numerous extensions to the original model. A great number of studies have applied the Judd-Ofelt theory to a wide range of rare-earth-doped materials, many of them with important applications in solid-state lasers, optical amplifiers, phosphors for displays and solid-state lighting, upconversion and quantum-cutting materials, and fluorescent markers. This paper takes the view of the experimentalist who is interested in appreciating the basic concepts, implications, assumptions, and limitations of the Judd-Ofelt theory in order to properly apply it to practical problems. We first present the formalism for calculating the wavefunctions of 4f electronic states in a concise form and then show their application to the calculation and fitting of 4f→4f transition intensities. The potential, limitations and pitfalls of the theory are discussed, and a detailed case study of LaCl3:Er3+ is presented.
| Original language | English |
|---|---|
| Pages (from-to) | 221-239 |
| Number of pages | 19 |
| Journal | Journal of Luminescence |
| Volume | 136 |
| DOIs | |
| Publication status | Published - 2013 |
| Externally published | Yes |
Keywords
- 4f transition intensities
- Intermediate coupling wavefunctions
- Judd-Ofelt theory
- Lifetimes and branching ratios
- Rare-earth spectroscopy
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