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1. 中国科学院长春光学精密机械与物理研究所, 激发态物理重点开放实验室,吉林 长春,130033
2. 吉林大学, 材料科学与工程学院,吉林 长春,130026
收稿日期:2002-09-11,
修回日期:2003-04-10,
纸质出版日期:2003-09-20
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彭洪尚, 宋宏伟, 陈宝玖, 王绩伟, 吕少哲, 黄世华. Y<sub>2</sub>O<sub>3</sub>:Eu<sup>3+</sup>纳米晶与体材料在高分辨光谱上的显著区别[J]. 发光学报, 2003,24(5): 531-534
PENG Hong-shang, SONG Hong-wei, CHEN Bao-jiu, WANG Ji-wei, L&#220; Shao-zhe, HUANG Shi-hua. Remarkable Spectral Difference between Nanocrystalline Y<sub>2</sub>O<sub>3</sub>:Eu<sup>3+</sup> and Bulk Ones[J]. Chinese Journal of Luminescence, 2003,24(5): 531-534
彭洪尚, 宋宏伟, 陈宝玖, 王绩伟, 吕少哲, 黄世华. Y<sub>2</sub>O<sub>3</sub>:Eu<sup>3+</sup>纳米晶与体材料在高分辨光谱上的显著区别[J]. 发光学报, 2003,24(5): 531-534 DOI:
PENG Hong-shang, SONG Hong-wei, CHEN Bao-jiu, WANG Ji-wei, L&#220; Shao-zhe, HUANG Shi-hua. Remarkable Spectral Difference between Nanocrystalline Y<sub>2</sub>O<sub>3</sub>:Eu<sup>3+</sup> and Bulk Ones[J]. Chinese Journal of Luminescence, 2003,24(5): 531-534 DOI:
报道了Y
2
O
3
:Eu
3+
纳米晶与体材料在光谱上的显著区别。除了相同于Y
2
O
3
:Eu
3+
体材料在580.6nm处的激发峰外
Y
2
O
3
:Eu
3+
纳米晶在579.9nm处出现了一新的较宽激发线。并且
该激发线的寿命要稍短于580.6nm的激发线。579.9nm激发线被归因于靠近纳米晶表面的Eu
3+
的发光。纳米晶中存在大量的表面缺陷
表面的晶体场因而发生退化
从而使得4f组态的电子能级发生移动。
In this paper
spectral difference between nanocrystalline yttria doped with europium (Y
2
O
3
:Eu
3+
) and the bulk ones was reported. Besides a 580.6nm line similar to that in the bulk Y
2
O
3
:Eu
3+
a new broad excitation line at 579.9nm was observed in the excitation spectra of nanocrystals (NCs). The 579.9nm peak relative to the 580.6nm one decreases a little as temperature increases. The fluorescent lifetime excited by 579.9nm line became slightly shorter than that of the 580.6nm line. We suggest that in nanocrystalline Y
2
O
3
:Eu
3+
the broader 579.9nm excitation peak originates from the luminescence of Eu
3+
ions near the surface
and the 580.6nm one from the internal Eu
3+
ions. The surface to volume ratio is quite small (1%) in the micrometer particles
while it increases significantly as the particle size decreases to several nanometers. This will lead the surface effects to be effective. As well known
the energies of electrons in 4f states of rare earth ions are affected by the crystal field. In nanocrystals
rare earth ions near the particle surface are at the sites microscopically inequivalent with those close to the center. Their energy levels may shift
and the degenerated spectral lines in the bulk sample may split. Due to the appearance of numerous surface defects the crystal field in the surface of nanoparticles degenerates and the emission of 5D
o
7
Fj
shifts. Because the local environments surrounding Eu
3+
ions near the surface are more disordered and surface defects may act as nonradiative transition channels
the width of the 579.9nm line is broader and the fluorescent lifetime becomes shorter.
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