CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES |
Prev
Next
|
|
|
Full-profile fitting of emission spectrum to determine transition intensity parameters of Yb3+: GdTaO4 |
Qingli Zhang(张庆礼)1, Guihua Sun(孙贵花)1, Kaijie Ning(宁凯杰)1, Chaoshu Shi(施朝淑)2, Wenpeng Liu(刘文鹏)1, Dunlu Sun(孙敦陆)1, Shaotang Yin(殷绍唐)1 |
1 The Key Laboratory of Photonic Devices and Materials, Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei 230031, China;
2 Physics Department of the Science and Technology of China, Hefei 230026, China |
|
|
Abstract The Judd-Ofelt theoretic transition intensity parameters Atpk of luminescence of rare-earth ions in solids are important for the quantitative analysis of luminescence. It is very difficult to determine them with emission or absorption spectra for a long time. A “full profile fitting” method to obtain Atpk in solids with its emission spectrum is proposed, in which the contribution of a radiative transition to the emission spectrum is expressed as the product of transition probability, line profile function, instrument measurement constant and transition center frequency or wavelength, and the whole experimental emission spectrum is the sum of all transitions. In this way, the emission spectrum is expressed as a function with the independent variables intensity parameters Atpk, full width at half maximum (FWHM) of profile functions, instrument measurement constant, wavelength, and the Huang-Rhys factor S if the lattice vibronic peaks in the emission spectrum should be considered. The ratios of the experimental to the calculated energy lifetimes are incorporated into the fitting function to remove the arbitrariness during fitting Atpk and other parameters. Employing this method obviates measurement of the absolute emission spectrum intensity. It also eliminates dependence upon the number of emission transition peaks. Every experiment point in emission spectra, which usually have at least hundreds of data points, is the function with variables Atpk and other parameters, so it is usually viable to determine Atpk and other parameters using a large number of experimental values. We applied this method to determine twenty-five Atpk of Yb3+ in GdTaO4. The calculated and experiment energy lifetimes, experimental and calculated emission spectrum are very consistent, indicating that it is viable to obtain the transition intensity parameters of rare-earth ions in solids by a full profile fitting to the ions' emission spectrum. The calculated emission cross sections of Yb3+:GdTaO4 also indicate that the F-L formula gives larger values in the wavelength range with reabsorption.
|
Received: 22 June 2016
Revised: 28 July 2016
Accepted manuscript online:
|
PACS:
|
78.55.-m
|
(Photoluminescence, properties and materials)
|
|
78.60.Lc
|
(Optically stimulated luminescence)
|
|
75.10.Dg
|
(Crystal-field theory and spin Hamiltonians)
|
|
Fund: Project supported by the National Natural Science Foundation of China (Grant Nos. 51172236, 51502292, 51272254, 51102239, 61205173, and 61405206). |
Corresponding Authors:
Qingli Zhang
E-mail: zql@aiofm.ac.cn
|
Cite this article:
Qingli Zhang(张庆礼), Guihua Sun(孙贵花), Kaijie Ning(宁凯杰), Chaoshu Shi(施朝淑), Wenpeng Liu(刘文鹏), Dunlu Sun(孙敦陆), Shaotang Yin(殷绍唐) Full-profile fitting of emission spectrum to determine transition intensity parameters of Yb3+: GdTaO4 2016 Chin. Phys. B 25 117802
|
[1] |
Judd B R 1962 Phys. Rev. 127 750
|
[2] |
Ofelt G S 1962 J. Chem. Phys. 37 511
|
[3] |
Reid M F and Richardson F S 1984 J. Chem. Phys. 88 3579
|
[4] |
Newman D J and Balasubramanian G 1975 J. Phys. C:Solid State Phys. 8 37
|
[5] |
Reid M F and Richardson F S 1983 J. Chem. Phys. 79 5735
|
[6] |
Reid M F, Dallara J J and Richardson F S 1983 J. Chem. Phys. 79 5743
|
[7] |
Newman D J and Ng B 2000 Crystal Field Handbook (New York:Cambdrige Univeristy Press) p. 208
|
[8] |
Judd B R 1963 Operator Techniques and Atomic Spectroscopy(New York, San Francisco, Toronto, London:McGraw-Hill Book Company) p. 42, p. 72
|
[9] |
Theo H 2005 International Tables for Crystallography, Volume A:Space-Group Symmetry (5th edn.) (Dordrecht:Springer) p. 195
|
[10] |
Huang K 1981 Adv. Phys. 1 31
|
[11] |
Zhang Q L, Wang X M, Yin S T and Jiang H H 2008 Eng. Sci. 10 35
|
[12] |
Zhang Q L, Ning K J, Ding L H, Liu W P, Sun D L, Jiang H H and Yin S T 2013 Chin. Phys. B 22 067105
|
[13] |
Krupke W F 1966 Phys. Rev. 145 325
|
[14] |
Dorenbos P 2000 J. Luminun. 91 155
|
[15] |
Goldner P, Schaudel B and Prassas M 2002 Phys. Rev. B 65 054103
|
[16] |
Krupke W F and Gruber J B 1965 Phys. Rev. B 139 A2008
|
[17] |
Ma Z 2005 Handbook of Modern Applied Mathematics, Computational and Numerical Analysis (Beijing:Tsinghua University press) p. 554
|
[18] |
Liu W 2009 Preparation, Single Crystal Growth and Luminescence Properties of New Type Scintillators with High Density (Hefei:Ph D Dissertation of Chinese Academy of Sciences) p. 92
|
[19] |
Patel F D, Honea E C, Speth J, Payne S A, Hutcheson R and Equall R 2001 IEEE J. Quantum Electron. 37 135
|
[20] |
Orazio S 1998 Principles of Lasers (4th edn.) (New York and London:Plenum Press) p. 339
|
No Suggested Reading articles found! |
|
|
Viewed |
|
|
|
Full text
|
|
|
|
|
Abstract
|
|
|
|
|
Cited |
|
|
|
|
Altmetric
|
blogs
Facebook pages
Wikipedia page
Google+ users
|
Online attention
Altmetric calculates a score based on the online attention an article receives. Each coloured thread in the circle represents a different type of online attention. The number in the centre is the Altmetric score. Social media and mainstream news media are the main sources that calculate the score. Reference managers such as Mendeley are also tracked but do not contribute to the score. Older articles often score higher because they have had more time to get noticed. To account for this, Altmetric has included the context data for other articles of a similar age.
View more on Altmetrics
|
|
|