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1.兰州大学 核科学与技术学院 兰州 730000
2.西北核技术研究所 西安 710024
Received:26 May 2016,
Revised:13 July 2016,
Published:2016-10
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Di YANG, Mengli SUN, Wei YUAN, et al. Study on photoluminescence and Raman scattering in GaAs by ion irradiation[J]. Nuclear techniques, 2016, 39(10): 100201
Di YANG, Mengli SUN, Wei YUAN, et al. Study on photoluminescence and Raman scattering in GaAs by ion irradiation[J]. Nuclear techniques, 2016, 39(10): 100201 DOI: 10.11889/j.0253-3219.2016.hjs.39.100201.
利用250 keV质子和4.5 MeV氪离子(Kr
17+
)辐照未掺杂GaAs,注量分别为1
&
#215;10
12
-3
&
#215;10
14
cm
-2
和1
&
#215;10
11
-3
&
#215;10
14
cm
-2
,使用光致发光谱和拉曼散射谱分析表征。发光谱的结果表明,随着剂量增大,质子辐照后的C
As
峰及其声子伴线逐渐减弱,913 nm处的复合缺陷峰则先增大后减小,此峰与材料制备时的Cu掺杂无关。Kr离子辐照后本征发光峰则完全消失。拉曼散射谱的结果表明,相比于质子辐照,Kr离子辐照后LO声子峰峰位向低频方向移动,出现非对称性展宽,晶体结构发生明显改变。质子和Kr离子辐照效应的差异是由于移位损伤相差至少三个量级造成的。最后采用多级损伤累积(Multi-step damage accumulation,MSDA)模型得到了材料内缺陷的演化过程,并很好地解释了随损伤剂量增大GaAs光学性能及晶体结构的变化趋势。
Background:
2
GaAs is widely used as the second generation semiconductor material in the fields of aerospace and radiation detection.
Purpose:
2
Study of the irradiation effects of GaAs is of guiding significance for the evaluation of the radiation resistance of GaAs devices.
Methods:
2
Semi-insulating GaAs were irradiated by 250-keV H+ and 4.5-MeV Kr
17+
ions with fluences ranging respectively from 1
&
#215;1012 cm
-2
to 3
&
#215;1014 cm
-2
and 3
&
#215;1011 cm
-2
to 3
&
#215;1014cm
-2
. Photoluminescence (PL) spectrum and Raman scattering spectra were used to measure GaAs samples before and after irradiation.
Results:
2
PL spectrum shows that the intensity of C
As
peaks and phonon replicas decrease with increasing fluence of H+ irradiation. The IGa-VAs peak in 913 nm was increased at lower fluence and decreased at higher fluences. But all the peaks completely disappeared with Kr
17+
irradiation. The results of Raman spectra show that the longitudinal-optical (LO) phonon peak at 295-cm
-1
slides towards the low-frequency side and broadens its width asymmetrically by Kr
17+
irradiation
while it has no obvious change by proton irradiation.
Conclusion:
2
The difference between the effect of proton and Kr
17+
irradiation is due to the difference of the displacement damage by three orders of magnitude at least. The evolution process of damage defects in GaAs is obtained by using Multi-step damage accumulation (MSDA) model
and then the trends of optical properties and crystalline structure are well explained.
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