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Judd–Ofelt theory
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Judd–Ofelt theory : ウィキペディア英語版
Judd–Ofelt theory

Judd–Ofelt theory is a theory in physical chemistry describing the intensity of electron transitions within the 4''f'' shell of rare earth ions in solids and solutions.〔〔
The theory was introduced independently in 1962 by Brian R. Judd of the University of California, Berkeley, and PhD candidate George S. Ofelt at Johns Hopkins University.〔 Their work was published in ''Physical Review'' and the ''Journal of Chemical Physics'', respectively.〔〔 Judd and Ofelt did not meet, however, until 2003 at a workshop in Lądek-Zdrój, Poland.〔
==Theory==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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