1. 广东工业大学 物理与光电工程学院,广东,广州,510006
2. 东源广工大现代产业协同创新研究院,广东,河源,517000
黄穗超(1990-),男,硕士研究生,主要研究方向为上转换发光材料
胡正发(1972-),男,副研究员,主要研究方向为热致、电致发光材料. E-mail:zhfhu@gdut.edu.cn
网络首发:2019-01-25,
纸质出版:2019
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黄穗超, 胡正发, 张伟. 上转换材料LiY(MoO4)2:Yb3+/Er3+的光学特性以及温度传感特性的研究[J]. 广东工业大学学报, 2019, 36(1): 75-80. DOI: 10.12052/gdutxb.180064.
Huang Sui-chao, Hu Zheng-fa, Zhang Wei. The Temperature-Sensor and Optical Properties of Up-Conversion Phosphor LiY(MoO4)2:Yb3+/Er3+[J]. 2019, 36(1): 75-80. DOI: 10.12052/gdutxb.180064.
黄穗超, 胡正发, 张伟. 上转换材料LiY(MoO4)2:Yb3+/Er3+的光学特性以及温度传感特性的研究[J]. 广东工业大学学报, 2019, 36(1): 75-80. DOI: 10.12052/gdutxb.180064. DOI:
Huang Sui-chao, Hu Zheng-fa, Zhang Wei. The Temperature-Sensor and Optical Properties of Up-Conversion Phosphor LiY(MoO4)2:Yb3+/Er3+[J]. 2019, 36(1): 75-80. DOI: 10.12052/gdutxb.180064. DOI:
采用中温固相反应法合成了发光材料LiY(MoO
4
)
2
:Yb
3+
/Er
3+
材料具有明显的上转换发光特性. 通过X射线衍射仪、荧光光谱对荧光粉的晶体结构以及发光学特性进行了研究. 在980 nm激光的激发下
LiY(MoO
4
)
2
:Yb
3+
/Er
3+
在500~575 nm波长范围内出现很强的绿色发射带
主要是源自Er
3+
离子
2
H
11/2
/
4
S
3/2
→
4
I
15/2
的能级辐射跃迁. 研究发现其在不同功率的激发下能实现光色调控. 在298~513 K温度范围内
通过测量其在
2
H
11/2(1)
→
4
I
15/2
和
4
S
3/2(1)
→
4
I
15/2
处的荧光强度比
数据拟合图像表明
2
H
11/2(1)
/
4
S
3/2(1)
热耦合能级上的布居数遵循玻尔兹曼分布
相对灵敏度在298 K达到最大值1.785% K
–1
绝对灵敏度在约473 K达到最大值263.20×10
–4
K
–1
并且热能级
2
H
11/2(1)
/
4
S
3/2(1)
之间的能隙Δ
E
为756.71±27.48 cm
–1
. 基于以上分析
LiY(MoO
4
)
2
:Yb
3+
/Er
3+
荧光粉在温度传感器上具有很好的前景.
The phosphors LiY(MoO
4
)
2
:Yb
3+
/Er
3+
with remarkable up-conversion emission character were synthesized by means of high-temperature solid state reaction method. Experiments were carried out to determine the crystal structure
up-conversion emission optical properties and temperature sensing of the phosphors. Under 980 nm laser
the LiY(MoO
4
)
2
:Yb
3+
/Er
3+
exhibits an intensive green emission bands which can be assigned to
2
H
11/2
/
4
S
3/2
→
4
I
15/2
transitions. The temperature sensing properties were studied by measuring the fluorescence intensity ratio of the
2
H
11/2(1)
and
4
S
3/2(1)
emitting energy levels in the temperature range from 298 to 513 K. The maximum relative sensitivity was 1.785% K
-1
at 298 K and the maximum absolute sensitivity reach to 263.20×10
−4
K
−1
at 473 K
and the calculated energy gap Δ
E
between
2
H
11/2(1)
and
4
S
3/2(1)
levels was 756.71±27.48 cm
−1
suggesting that the present phosphor is a suitable candidate for optical temperature sensors.
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