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1. 中国科学院长舂光学精密机械与物理研究所, 激发态物理重点实验室, 吉林, 长春, 130033
2. 吉林省医药职工中等专业学校, 吉林, 长春, 130051
收稿日期:2004-03-22,
修回日期:2004-05-20,
纸质出版日期:2004-11-20
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杨林梅, 宋宏伟, 于立新, 刘钟馨, 吕少哲, 马丽群. Y<sub>2</sub>O<sub>3</sub>:Ho/Yb纳米晶的上转换发光性质[J]. 发光学报, 2004,25(6): 710-714
YANG Lin-mei, SONG Hong-wei, YU Li-xin, LIU Zhong-xin, L&#220; Shao-zhe, MA Li-qun. Upconversion Luminescence in Nanocrystalline Y<sub>2</sub>O<sub>3</sub>:Ho/Yb[J]. Chinese Journal of Luminescence, 2004,25(6): 710-714
杨林梅, 宋宏伟, 于立新, 刘钟馨, 吕少哲, 马丽群. Y<sub>2</sub>O<sub>3</sub>:Ho/Yb纳米晶的上转换发光性质[J]. 发光学报, 2004,25(6): 710-714 DOI:
YANG Lin-mei, SONG Hong-wei, YU Li-xin, LIU Zhong-xin, L&#220; Shao-zhe, MA Li-qun. Upconversion Luminescence in Nanocrystalline Y<sub>2</sub>O<sub>3</sub>:Ho/Yb[J]. Chinese Journal of Luminescence, 2004,25(6): 710-714 DOI:
采用燃烧法制备了不同尺寸和不同掺杂浓度的Y
2
O
3
:Ho/Yb纳米晶
并系统地研究了颗粒尺寸对Y
2
O
3
:Ho/Yb纳米晶发光性质的影响。研究发现
随着尺寸的减小
发射强度和荧光分支比均发生了显著变化
Ho
3+
的整体发射强度降低
但
5
F
5
5
I
8
的红光发射比
5
S
2
(
5
F
4
)
5
I
8
的绿光发射的荧光分支比增强。尺寸减小
表面原子更易吸附空气中的水和二氧化碳
引入一些较大的振动模式
从而增大了无辐射跃迁的速率
荧光分支比随尺寸的变化被归因于表面效应引起的无辐射弛豫过程
5
S
2
(5F
4
)
5
F
5
和
5
I
6
5
I
7
的增强。
Y
2
O
3
:Ho/Yb nanocrystals have been prepared by combustion method. The nano-crystals size was estimated by X-ray diffraction. Green emissions near 549 nm and red emissions near 668 nm were observed under 488 nm and 980 nm excitation
which were associated with
5
S
2
(
5
F
4
)
5
I
8
and
5
F
5
5
I
8
transitions of Ho
3+
that required two-step energy transfer (ET) from Yb
3+
ions. The intensity ratio of red light to green light varied obviously with the nanocrystals size
which should be due to surface defects. The smaller the size was
the weaker the emission intensity became. As the same time
the ratio of red light intensity to green light intensity increased obviously with the decrease of particle size. As the particle size decreased
a great number of surface defects were involved. These defects
which acted as nonradiative transition channels
led the decrease of the emission intensity. On the other hand
the surface of the powders absorbed the CO
2
and the H
2
Oin the air. So large vibrational modes could be produced
which offered the probability for depopulating of the excited states nonradiatively. Thus
the nonradiative relaxation rates from
5
S
2
(
5
F
4
) to
5
F
5
became much faster. As a result the ratio of red light intensity to green light intensity decreased. Two nonradiative relaxations processes
5
S
2
(
5
F
4
)
5
F
5
and
5
I
6
5
I
7
are involved in upconversion luminescence
but only
5
S
2
(
5
F
4
)
5
F
5
in downconversion. So the increase of emission intensity ratio is more prominent in upconversion luminescence than downconversion luminescence.
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