TY - JOUR
T1 - Study on upconversion luminescence and luminescent dynamics of 20%Yb 3+, 0.5%Tm 3+ co-doped YF 3and GdF 3 nanocrystals
AU - Cao, Chunyan
AU - Qin, Weiping
AU - Zhang, Jisen
PY - 2010/3
Y1 - 2010/3
N2 - 20%Yb 3+, 0.5%Tm 3+ co-doped YF 3 and GdF 3 were synthesized through a facile hydrothermal method. After annealing under an argon atmosphere, the sizes and morphologies of the two samples were characterized by field emission scanning electron microscopy, and the phase and crystallization were analyzed by X-ray diffraction. With a 980 nm continuous wave laser diode as the excitation source, blue and ultraviolet upconversion emissions in the wavelength range of 260-510 nm of Tm 3+ and Gd 3+/Tm 3+ ions were recorded. Under the same excitation conditions, the upconversion emission spectra of the two nanocrystals were compared and analyzed. Gd 3+ in the ground state cannot absorb 980 nm photons directly because of the large energy gap between the ground state 8S 7/2 and the first excited state 6P 7/2. In the 20%Yb 3+, 0.5%Tm 3+ co-doped GdF3 nanocrystals, the excited states 6l j of Gd 3+ can be populated through the energy transfer 3P 2 → 3H 6 (Tm 3+): 8S 7/2 → 6l j(Gd 3+), meaning that Yb 3+ acted as primary sensitizers and Tm 3+ acted as secondary sensitizers, transferred energies to host material Gd 3+ and resulted in the ultraviolet upconversion emission of the host ions. In this article, the upconversion luminescent dynamics were studied at the onset of a 980 nm pulsed laser from an optical parametric oscillator pumped by a 10 ns pulsed Nd:YAG laser, too
AB - 20%Yb 3+, 0.5%Tm 3+ co-doped YF 3 and GdF 3 were synthesized through a facile hydrothermal method. After annealing under an argon atmosphere, the sizes and morphologies of the two samples were characterized by field emission scanning electron microscopy, and the phase and crystallization were analyzed by X-ray diffraction. With a 980 nm continuous wave laser diode as the excitation source, blue and ultraviolet upconversion emissions in the wavelength range of 260-510 nm of Tm 3+ and Gd 3+/Tm 3+ ions were recorded. Under the same excitation conditions, the upconversion emission spectra of the two nanocrystals were compared and analyzed. Gd 3+ in the ground state cannot absorb 980 nm photons directly because of the large energy gap between the ground state 8S 7/2 and the first excited state 6P 7/2. In the 20%Yb 3+, 0.5%Tm 3+ co-doped GdF3 nanocrystals, the excited states 6l j of Gd 3+ can be populated through the energy transfer 3P 2 → 3H 6 (Tm 3+): 8S 7/2 → 6l j(Gd 3+), meaning that Yb 3+ acted as primary sensitizers and Tm 3+ acted as secondary sensitizers, transferred energies to host material Gd 3+ and resulted in the ultraviolet upconversion emission of the host ions. In this article, the upconversion luminescent dynamics were studied at the onset of a 980 nm pulsed laser from an optical parametric oscillator pumped by a 10 ns pulsed Nd:YAG laser, too
KW - 0.5% tm co-doped gdf
KW - 0.5%Tm co-doped yf
KW - 20%Yb
KW - Luminescent dynamics
KW - Upconversion
UR - http://www.scopus.com/inward/record.url?scp=77955002726&partnerID=8YFLogxK
U2 - 10.1166/jnn.2010.2054
DO - 10.1166/jnn.2010.2054
M3 - Article
AN - SCOPUS:77955002726
SN - 1533-4880
VL - 10
SP - 1900
EP - 1903
JO - Journal of Nanoscience and Nanotechnology
JF - Journal of Nanoscience and Nanotechnology
IS - 3
ER -