Investigation of doped calcium aluminosilicate glass: A coupling between thermal-expansion and thermal-diffusion models for assessment of nonradiative relaxation time and characteristic diffusion time
J. Appl. Phys. 106, 093105 (2009); doi:10.1063/1.3253580
Published 6 November 2009
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This paper discusses the use of photoacoustic models to obtain the nonradiative relaxation time (
) and characteristic diffusion time (
) for a sample showing visible absorption bands from fluorescent ion-doped low-silica calcium aluminosilicate glass. Two models allowing phase shift analyses, the thermal-expansion and thermal-diffusion models, are briefly reviewed. These models have limitations when the photoacoustic signal depends on both factors, in a coupling mechanism. An alternative model is proposed to take both thermal expansion and thermal diffusion into account with a single temperature solution for the heat-coupled differential equation. This model is simulated for absorbing samples near the thermally thick region. The model is applied to Eu–V codoped glass showing intermediate signal dependence from
−1.0 to
−3/2. The nonradiative time and characteristic diffusion time are derived with 33<
(ms)<39, and 
(ms)~70 ms for the Eu-ion and 340<
(ms)<710 for the V-ion. Four absorption bands were analyzed (280, 350, 420, and 600 nm), which showed a signal dependence from
−1.1 to
−1.52. Absorption coefficients were derived from 
in the range of 15<
(cm−1)<51, which agreed fairly well with spectrophotometer data for the same ions.
©2009 American Institute of Physics
) and characteristic diffusion time (
) for a sample showing visible absorption bands from fluorescent ion-doped low-silica calcium aluminosilicate glass. Two models allowing phase shift analyses, the thermal-expansion and thermal-diffusion models, are briefly reviewed. These models have limitations when the photoacoustic signal depends on both factors, in a coupling mechanism. An alternative model is proposed to take both thermal expansion and thermal diffusion into account with a single temperature solution for the heat-coupled differential equation. This model is simulated for absorbing samples near the thermally thick region. The model is applied to Eu–V codoped glass showing intermediate signal dependence from
−1.0 to
−3/2. The nonradiative time and characteristic diffusion time are derived with 33<
(ms)<39, and 
(ms)~70 ms for the Eu-ion and 340<
(ms)<710 for the V-ion. Four absorption bands were analyzed (280, 350, 420, and 600 nm), which showed a signal dependence from
−1.1 to
−1.52. Absorption coefficients were derived from 
in the range of 15<
(cm−1)<51, which agreed fairly well with spectrophotometer data for the same ions.
©2009 American Institute of Physics
| History: | Received 31 August 2009; accepted 22 September 2009; published 6 November 2009 |
| Permalink: |
http://link.aip.org/link/?JAPIAU/106/093105/1 |
KEYWORDS and PACS
aluminosilicate glasses,
calcium compounds,
doping,
fluorescence,
nonradiative transitions,
photoacoustic effect,
thermal diffusion,
thermal expansion
- 78.55.Qr
Photoluminescence in amorphous materials - 65.40.De
Thermal expansion; thermomechanical effects (crystalline solids) - 66.70.Hk
Nonelectronic thermal conduction and heat-pulse propagation in glasses and polymers - 65.60.+a
Thermal properties of amorphous solids and glasses - 78.20.Hp
Piezo-, elasto-, and acoustooptical effects (bulk materials/thin films) - YEAR: 2009
PUBLICATION DATA
0021-8979 (print)
1089-7550 (online)
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