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1.
研究了Al掺杂对采用直流磁控溅射方法制备的ZnO薄膜结构及光学性能的影响。X射线衍射结果揭示薄膜具有良好的C轴择优取向生长特性,同时,衬底温度对它们的透射谱和荧光谱有着明显影响,所有薄膜都有大于86%的可见光透过率和陡峭的本征吸收边,但ZAO薄膜的光学透过率略低。Al掺杂导致了更宽的光学带隙,光致发光光谱显示ZnO具有较强的近带本征吸收峰和深能级发射峰,但Al掺杂使得深能级发射峰降低。随着衬底温度的升高,近带边吸收峰蓝移,与光学带隙Eg变化趋势一致。  相似文献   

2.
射频磁控溅射制备ZnO光波导薄膜   总被引:1,自引:4,他引:1  
采用射频磁控溅射技术在石英玻璃上制备出了具有高度c轴择优取向的ZnO薄膜。利用X射线衍射(XRD)、背散射分析(RBS)、棱镜耦合等技术对其结构、光波导性质进行研究,结果表明减小溅射压强有利于提高薄膜的结晶质量,增强薄膜的c轴择优取向。溅射压强越小,薄膜越厚,薄膜的有效折射率越接近晶体材料的折射率。  相似文献   

3.
采用脉冲沉积(PLD)法在石英玻璃衬底上制备了Zn1-xCdxO薄膜,X射线衍射仪(XRD)结果表明,所制备的Zn1-xCdxO薄膜具有与ZnO同样的六角纤锌矿结构,且薄膜具有沿着(002)晶面择优取向生长特征,随着Cd掺杂浓度(x)的增加,衍射峰(002)向小角度方向移动,晶格常数增加。光致发光光谱表明Zn1-xCdxO薄膜随着Cd的掺杂浓度的增加使光学带隙逐渐变窄了,且控制掺入量就可以实现ZnO薄膜禁带宽度在一定范围内连续可调。  相似文献   

4.
采用射频磁控溅射技术在不同溅射功率下制备了CdSe薄膜,并利用X射线衍射仪(XRD)、场发射扫描电子显微镜(FESEM)、能量色散X射线光谱仪(EDAX)、紫外可见近红外(UV-VIS-NIR)分光光度计和霍尔效应测试仪研究了溅射功率对薄膜的结构和光电学性质的影响.研究表明:增加溅射功率有利于增强薄膜的结晶性能;随着溅射功率的增加,薄膜的光学带隙和电阻率逐渐减小,载流子浓度逐渐增加,即薄膜的光电性能不断增强.该研究结果可为CdSe薄膜在光电器件方面的应用提供参考.  相似文献   

5.
采用RF磁控溅射法,在单晶硅衬底上生长出高质量的(002)晶面取向的ZnO薄膜.利用X射线衍射分析(XRD)、原子力显微镜(AFM)、光栅光谱仪等技术研究了沉积温度对ZnO薄膜的结构、应力状态、表面形貌和发光性能的影响.研究结果表明,在射频功率为100W时所制备的ZnO薄膜当沉积温度为500℃时能获得最佳的c轴取向和最小半高宽,此时ZnO薄膜具有较小的压应力和较好的紫外发光性.  相似文献   

6.
采用溶胶-凝胶法在单晶硅Si(100)衬底上制备了ZnO薄膜,研究了退火温度对ZnO结构和光学性能的影响。实验发现,退火可以明显地改善ZnO薄膜的结构和光学性能。随着退火温度的升高,ZnO薄膜的晶粒增大,同时在室温下观察到明显的紫外发光现象,其紫外PL谱峰值变强,并有红移现象。  相似文献   

7.
采用射频磁控溅射法在Si和Ti合金基体上沉积出类金刚石(DLC)薄膜.利用拉曼光谱仪、划痕仪和扫描电子显微镜分析了DLC薄膜的结构、膜基附着力和表面形貌.结果表明:射频磁控溅射法能够制备出表面平整、结构致密的DLC薄膜;同时基体材料的不同不会影响DLC薄膜的键合结构,Si基体上涂层附着力为30N,Ti基体上膜基结合力大于40 N.  相似文献   

8.
采用射频磁控溅射方法在玻璃和Si(111)衬底上制备了碲化镉(CdTe)薄膜,并研究了溅射功率对薄膜的结构、光学和电学性能的影响.X射线衍射分析表明,所有样品均沿(111)面择优取向; 平均晶粒尺寸随溅射功率的增加而增加,即从73.0 nm(70 W)增加到123.6 nm(110 W).紫外 - 可见 - 近红外光谱分析表明, CdTe薄膜在可见光范围内具有较高的吸光度; 薄膜的带隙随着溅射功率的增加而减小,最小值为1.38 eV.CdTe薄膜的导电性随溅射功率的增加而明显增强,当溅射功率为110 W时电阻率仅为21.5 Ω?cm.该研究结果可为制备高导电性和高吸收率的半导体薄膜提供参考.  相似文献   

9.
氮化铝(Al N)是一种宽禁带深紫外半导体材料,其良好的性能可作为紫外固态光源。采用射频磁控溅射法,在p型Si(100)衬底上制备了Al N薄膜。通过X射线衍射分析(XRD)、紫外-可见光光谱(UV-Vis)、场发射测试对制备的Al N薄膜进行了测试分析,针对薄膜生长特性对光吸收的影响及其场发射性能进行了研究。结果显示:在Si衬底上成功的制备了高度(002)取向的Al N薄膜,薄膜在230~250nm间有强紫外吸收,阈值电场为6.39V/μm。场发射测试结果表明,磁控溅射法制备的Al N薄膜具备良好的场发射性。  相似文献   

10.
TiO2是作为一种宽禁带半导体材料可作为紫外器件,但因其间接带隙结构、禁带宽度仅为3.0eV等特点,严重影响其应用范围。本文利用共溅射技术,通过Zn掺杂,在K9玻璃基底上制备了Ti-Zn-O复合薄膜,并研究了Zn溅射功率对其结构及光学性质的影响。结果显示:所制备的薄膜为ZnTiO3和不饱和TiO2的复合结构,随着Zn粒子的溅射能量增加,晶粒尺寸和表面粗糙度增加,并可将薄膜本征吸收边蓝移至3.61eV。  相似文献   

11.
ZnO thin films were prepared by direct current(DC) reactive magnetron sputtering under different oxygen partial pressures And then the samples were annealed in vacuum at 450 ℃. The effects of the oxygen partial pressures and the treatment of annealing in vacuum on the photoluminescence and the concentration of six intrinsic defects in ZnO thin films such as oxygen vacancy(Vo), zinc vacancy(VZn), antisite oxygen(OZn), antisite zinc(Zno), interstitial oxygen(Oi) and interstitial zinc(Zni) were studied. The results show that a green photoluminescence peak at 520 nm can be observed in all the samples, whose intensity increases with increasing oxygen partial pressure; for the sample annealed in vacuum, the intensity of the green peak increases as well. The green photoluminescence peak observed in ZnO may be attributed to zinc vacancy, which probably originates from transitions between electrons in the conduction band and zinc vacancy levels, or from transitions between electrons in zinc vacancy levels and up valence band.  相似文献   

12.
The microstructural,optical,and magnetic properties and room-temperature photoluminescence(PL) of Mn-doped ZnO thin films were studied.The chemical compositions were examined by energy dispersive X-ray spectroscopy(EDS) and the charge state of Mn ions in the ZnO:Mn films was characterized by X-ray photoelectronic spectrometry(XPS).From the X-ray diffraction(XRD) data of the samples,it can be found that Mn doping does not change the orientation of ZnO thin films.All the films prepared have a wurtzite stru...  相似文献   

13.
This study investigated the process parameter effects on the structural and optical properties of ZnO thin film using radio frequency (RF) magnetron sputtering on amorphous glass substrates. The process parameters included RF power and working pressure. Results show that RF power was increased to promote the crystalline quality and decrease ZnO thin film defects. However, when the working pressure was increased to 3 Pa the ZnO thin film crystalline quality became worse. At a 200 W RF power and 1 Pa working pressure, the ZnO thin film with an optical band gap energy of 3.225 eV was obtained. Supported by the National Natural Science Foundation of China (Grant Nos. 50772006, 10432050)  相似文献   

14.
Several batches of NiCr alloy thin films with different thickness were prepared in a multi-targets magnetron sputtering apparatus by changing sputtering time while keeping sputtering target power of Ni and Cr fixed. Then the as-deposited films were characterized by energy-dispersive X-Ray spectrometer (EDX), Atomic Force Microscope (AFM) and four-point probe (FPP) to measure surface grain size, roughness and sheet resistance. The film thickness was measured by Alpha-Step IQ Profilers. The thickness dependence of surface roughness, lateral grain size and resistivity was also studied. The experimental results show that the grain size increases with film thickness and the surface roughness reaches the order of nanometer at all film thickness. The as-deposited film resistivity decreases with film thickness.  相似文献   

15.
以Zn-Al(Al:2wt.%)合金为溅射靶材,采用直流反应磁控溅射的方法,在普通玻璃衬底上制备Al掺杂ZnO(AZO)薄膜。通过对衬底温度的调制,在较高衬底温度下(~280℃),无需经过常规溅射后腐蚀工艺过程,即可获得表面形貌具有特征陷光结构的AZO薄膜,其表面呈现类金字塔状,粗糙度RMS=65.831nm。通过测试薄膜的结构特性、表面形貌及其光电性能,详细地研究了衬底温度对AZO薄膜性能的影响。X射线衍射(XRD)和扫描电子显微镜(SEM)测试表明,所有样品均为多晶六角纤锌矿结构,薄膜呈(002)晶面择优生长,其表面形貌随衬底温度的不同而改变。衬底温度为200℃及其以上工艺条件下获得的AZO薄膜,在可见光及近红外范围的平均透过率大于90%,电阻率优于1.5×10-3Ωcm。  相似文献   

16.
采用射频磁控溅射方法,在Si(111)和玻璃基片上制备ZnO薄膜。研究衬底温度和基片类型对薄膜结构、表面形貌的影响。结果显示,所有ZnO薄膜沿c轴择优生长,同种基片类型上生长的薄膜,随着衬底温度升高,(002)衍射峰强度和表面粗糙度增高;相同衬底温度下生长的ZnO薄膜,Si基片上制备的薄膜(002)衍射峰强度和表面粗糙度小于玻璃片上的。基片类型影响薄膜应力状态,玻璃片上制备的ZnO薄膜处于张应变状态,Si基片上的薄膜处于压应变状态;对于同种基片类型上生长的ZnO薄膜,衬底温度升高,应力减小。Si衬底上、300℃下沉积的薄膜颗粒尺寸分布呈正态。  相似文献   

17.
Cu3N and Al Cu3N films were prepared with reactive magnetron sputtering method. The two films were deposited on glass substrates at 0.8 Pa N2 partial pressure and 100 ℃ substrate temperature by using a pure Cu and AI target, respectively. X-ray diffraction (XRD) measurements show that the un-doped film was composed of Cu3N crystallites with anti-ReO3 structure and adopted [111] preferred orientation. XRD shows that the growth of Al-doped copper nitride films (AlxCu3N) was affected strongly by doping AI, the intensity of [111] peak decreases with increasing the concentration of Al and the high concentration of Al could prevent the Cu3N from crystallization. AFM shows that the surface of AlCu3N film is smoother than that of Cu3N film. Compared with the Cu3N films, the resistivities of the Al-doped copper nitride films (AlxCu3N) have been reduced, and the microhardness has been enhanced.  相似文献   

18.
不同磁控溅射模式膜厚均匀性研究   总被引:9,自引:0,他引:9  
使用磁控溅射和非平衡磁控溅射方法,在玻璃基底上沉积钛膜。实验了在同等工艺条件下平衡和非平衡两种不同的工作模式对膜厚均匀性的影响。结果表明,靶基距是影响磁控溅射薄膜厚度均匀性的重要工艺参数,在一定范围内,随着靶基距的增大,膜厚分布均匀性有提高的趋势;磁场分布是影响两种磁控溅射膜厚分布差异的主要因素;非平衡磁控溅射膜厚均匀性随附加励磁线圈电流改变而变化。  相似文献   

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