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1. 大连理工大学, 物理系, 辽宁, 大连, 116023
2. 吉林大学, 电子科学与工程学院, 集成光电子学国家重点实验室, 吉林, 长春, 130023
收稿日期:2003-03-17,
修回日期:2003-05-19,
纸质出版日期:2004-03-20
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常玉春, 杨晓天, 王金忠, 王新强, 刘博阳, 刘大力, 胡礼忠, 杜国同. 等离子MOCVD系统生长ZnO薄膜掺N<sub>2</sub>和掺NH<sub>3</sub>特性比较[J]. 发光学报, 2004,25(2): 143-146
CHANG YU-chun, YANG Xiao-tian, WANG Jin-zhong, WANG Xin-qiang, LIU Bo-yang, LIU Da-Li, HU Li-zhong, DU Guo-tong. Comparing with the Characteristics of N<sub>2</sub> and NH<sub>3</sub> Doped ZnO Thin Films Grown by Plasma MOCVD System[J]. Chinese Journal of Luminescence, 2004,25(2): 143-146
常玉春, 杨晓天, 王金忠, 王新强, 刘博阳, 刘大力, 胡礼忠, 杜国同. 等离子MOCVD系统生长ZnO薄膜掺N<sub>2</sub>和掺NH<sub>3</sub>特性比较[J]. 发光学报, 2004,25(2): 143-146 DOI:
CHANG YU-chun, YANG Xiao-tian, WANG Jin-zhong, WANG Xin-qiang, LIU Bo-yang, LIU Da-Li, HU Li-zhong, DU Guo-tong. Comparing with the Characteristics of N<sub>2</sub> and NH<sub>3</sub> Doped ZnO Thin Films Grown by Plasma MOCVD System[J]. Chinese Journal of Luminescence, 2004,25(2): 143-146 DOI:
利用MOCVD方法生长了高质量的ZnO薄膜材料
分别通过N
2
和NH
3
对
c
面和
R
面蓝宝石衬底上生长的ZnO薄膜材料进行了掺杂行为研究.掺N
2
时
X射线衍射半峰全宽仅为0.148°
室温光荧光发光峰位于3.29eV
半峰全宽~100meV
电阻率由0.65Ω·cm增大到5×10
4
Ω·cm.掺NH
3
时
X射线衍射峰半峰全宽0.50°
样品为弱p型
电阻率为102Ω·cm
载流于浓度为1.69×10
16
cm
-3
.同时我们还观察到弱p型材料很容易退化成n型高阻材料.
ZnO is a multi-function direct wide-band semiconductor material with wurtzite structure.It has potential applications in varistors
phosphors
transparent electrode
optoelectronic devices
blue-purple light devices.n-type low resistivity ZnO is easy to obtain.However
the difficulty of high resistivity ZnO and p type ZnO must be resolved for the purpose of fabricating practical ZnO devices.Although many research groups are working on it
p-type ZnO problem has never been figured out.N is an effective p-type dopant for Ⅱ-Ⅵ group compounds.There are two effects when N is doped in ZnO thin films:providing a shadow acceptor energy level and decreasing concentration of Zn
i
atoms by combining with ZnO.Thus
it is possible to obtain high resistivity and p-type ZnO by doping N atoms in ZnO.There has two kinds of N source
N
2
and NH
3
.In this paper
the behaviors of N
2
and NH
3
doped in ZnO thin films are investigated.Firstly
N
2
was doped in ZnO thin films grown on c-plane sapphire substrate using plasma assisted MOCVD system.Plasma generator of plasma assisted MOCVD system is very efficient to dope N atoms into ZnO films and to obtain high resistivity ZnO thin films.The N
2
doped ZnO films have all of properties of ZnO and show high crystal quality
especially in optical properties
which show light-yellow body color.XRD measurement shows a high intensity peak at 2θ=34.6°with a FWHM of 0.148°
which is(002)peak of ZnO.The corresponding value of double-crystal XRD rocking-curve is 0.34°.The emitting peak locates at 3.29 eV in PL spectrum with a FWHM of 100meV.Compared with 0.65Ω·cm of undoped sample
the resistivity increases to 5×10
4
Ω·cm with N
2
doping.Secondly
the behavior of NH
3
doped ZnO grown on R-plane sapphire has been investigated.After optimized growth conditions
the XED result shows a high intensity peak at 2θ=56.30°with a FWHM of 0.50°
which is
<
110
>
peak of ZnO.The AFM photo shows that the surface of the film is very smooth.The roughness is about 3.01nm.Under different NH
3
flux
the sasple's
resistivity has different value as well as electrica1 conduction type.The p-type sample was obtained when NH
3
flux is 80 sccm with the resistivity of 102Ω·cm
observed by Hall measurement.Finally
we found that the p-type sample has the trend of turning to n-type.This maybe is due to instability of N-Zn bond in N doped ZnO which is investigated by XPS measurements.Consequently
behavior studies of N doping in ZnO are important to achieve high resistivity p-type ZnO thin films.Furthermore
it is maybe possible to obtain better results by annealing samples under protection of N
2
or NH
3
.
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