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1.
不同氧分压下直流反应溅射ZnO薄膜的结构和光学特性   总被引:1,自引:0,他引:1  
郑丁葳  倪晟  赵强  王基庆 《光学学报》2007,27(4):39-743
在室温,不同氧分压条件下,采用Zn靶直流反应溅射在石英衬底上制备了具有纤锌矿结构(002)择优取向的ZnO薄膜。薄膜的生长速率随氧分压的增大而减小,在20%-30%之间存在一个拐点,在此点之前,溅射产额减小的速率很快,而在此点之后,溅射产额减小的速率减慢了很多,当氧分压在30%以上时,溅射过程中Zn的氧化在靶表面就已经完成。通过单振子模型分析了薄膜的光学特性,采用X射线衍射的方法对薄膜的晶粒尺寸和应力进行分析。研究结果表明在氧分压20%以上时,薄膜在可见光波段具有较好的光学透明性和很高的电阻率。薄膜的光学折射率、晶面间距和内部应力均随着氧分压的增大而增大。并从薄膜生长机理上给出了理论解释。  相似文献   

2.
直流磁控反应溅射法制备大面积AZO薄膜的实验研究   总被引:1,自引:0,他引:1  
用锌铝合金靶在苏打玻璃上制备大面积AZO半导体透明薄膜,降低了靶材费用。实验中采用靶体旋转的直流磁控溅射工艺,提高了靶材利用率,实现了大面积均匀镀膜,并能获得定向生长的薄膜。文章介绍了采用该方法制备大面积薄膜的实验,并用X射线衍射仪、扫描电子显微镜等多种分析方法对大面积薄膜的结构、形貌、电学性能及光学性能进行分析,实验结果表明,采用合金靶做靶源,氩作工作气体,控制好氧气分压,大功率溅射可以获得定向性好、致密、均匀、透射率高、电阻率低的优质大面积(300 mm×300 mm)AZO薄膜。  相似文献   

3.
采用直流反应溅射的方法在具有立方织构的Ni基底上制备出了Y2O3隔离层,并研究了基带温度与H2O分压两个因素对Y2O3薄膜的织构取向以及表面形貌的影响。X射线衍射(XRD)结果和扫描电子显微镜(SEM)的分析表明,在温度为760℃,H2O分压为1.68×10-2Pa的条件下制备出的Y2O3薄膜具有强立方织构,平面内Φ扫描半高宽为7.07°,其表面均匀、致密、无裂纹。  相似文献   

4.
In掺杂ZnO薄膜的制备及其特性研究   总被引:13,自引:2,他引:13  
采用射频反应溅射技术在硅(100)衬底上制备了未掺杂和掺In的ZnO薄膜。掠角X射线衍射测试表明,实验中制备的掺In样品为ZnO薄膜。用X射线衍射仪、原子力显微镜和荧光分光光度计分别对两样品的结构、表面形貌和光致发光特性进行了表征,分析了In掺杂对ZnO薄膜的结构和发光特性的影响。与未掺杂ZnO薄膜相比,掺In ZnO薄膜具有高度的C轴择优取向,同时样品的晶格失配较小,与标准ZnO粉末样品之间的晶格失配仅为0.16%;掺In ZnO薄膜表面平滑,表面最大不平整度为7nm。在掺In样品的光致发光谱中观察到了波长位于415nm和433nm处强的蓝紫光双峰,对掺In样品的蓝紫双峰的发光机理进行了讨论,并推测出该蓝紫双峰来源于In替位杂质和Zn填隙杂质缺陷。  相似文献   

5.
蓝光ZnO薄膜的特性研究   总被引:2,自引:0,他引:2  
朋兴平  杨扬  耿伟刚  杨映虎  王印月 《发光学报》2005,26(4):531-534,i0002
采用反应溅射法在n型硅(100)衬底上制备了ZnO薄膜,分别用X射线衍射仪、原子力显微镜和荧光分光光度计对样品的结构、表面形貌和光致发光特性进行了表征。X射线衍射结果表明,实验中制备出了应变小的c轴择优取向的ZnO薄膜;原子力显微镜观察表明,薄膜表面平整,颗粒大小约为50nm,为柱状结构,颗粒垂直于硅衬底表面生长;在室温光致发光(PL)谱中观察到了波长位于434nm处的较窄的强蓝光发射峰,该蓝光峰的半峰全宽约为50meV。对蓝光峰的发光机制进行了讨论,并推断出该蓝光峰来源于电子从Zn填隙缺陷能级向价带顶跃迁。  相似文献   

6.
采用无催化脉冲激光沉积(PLD)方法,在InP(100)衬底上生长纳米ZnO柱状结构。采用扫描电子显微镜(SEM)、X射线衍射(XRD)以及光致发光(PL)谱等表征手段对ZnO纳米柱的形貌、晶体结构和光学特性进行了观察。SEM图像观察到ZnO纳米柱状结构具有一定的取向性;XRD测试在2θ=34.10°处观测到强的ZnO(002)衍射峰,证实ZnO纳米柱具有较好的c轴择优取向;室温PL谱在379nm处观察到了强的自由激子发射峰(半峰全宽为19nm),未探测到深能级跃迁发射峰,表明生长的纳米ZnO结构具有很高的光学质量。  相似文献   

7.
陈超  冀勇  郜小勇  赵孟珂  马姣民  张增院  卢景霄 《物理学报》2012,61(3):36104-036104
文章采用直流脉冲磁控反应溅射(DCPsputtering)技术,在不同氧氩比(GFR)条件下玻璃衬底上制备了一系列掺铝氧化锌(AZO)薄膜,并利用X射线衍射、扫描电子显微镜和分光光度计从宏观应力和微观晶格畸变的角度研究了GFR对薄膜结构、表面形貌和光学特性的影响.制备的多晶AZO薄膜呈现了明显的ZnO-(103)择优取向,这归结于3小时薄膜沉积过程中伴随的退火引起的薄膜晶面能转变.随着GFR的增大,AZO薄膜内宏观拉应力先增大到最大值,随后宏观压应力随着GFR的继续增大而增大.薄膜中的宏观应力明显随着GFR从拉应力向压应力转变.这与晶格微观畸变诱导的微观应力的研究结果趋势恰恰相反.随着GFR的增加,薄膜在可见光区的平均透射率先增加后减小,薄膜晶粒尺寸诱导的晶界散射是影响薄膜透射率的主导机制.  相似文献   

8.
采用射频磁控溅射方法制备了三明治结构ZnO紫外光电探测器,即在传统金属-半导体-金属(MSM)单层ZnO紫外光电探测器的基础上再铺设一层ZnO薄膜,从而构建三明治器件结构。三明治结构ZnO紫外光电探测器响应度在5V偏压下达到了0.05A/W,暗电流为1.44×10-5A,器件的整体性相比较传统单层ZnO紫外光电探测器得到了明显的改善。这主要归因于金属与半导体接触的耗尽区可以直接吸收入射光,提高了入射光的吸收效率,避免了传统上层电极对入射光的遮蔽作用。  相似文献   

9.
ZnO纳米块体材料的制备及其性能的研究   总被引:2,自引:0,他引:2  
采用连续成型方式压制了纳米ZnO素坯,考察了素坯密度、烧结时间、致密化温度等参数与 成型方式的关系.用场发射扫描电镜表征了烧结体微观组织特征.测定了ZnO纳米块体材料中 硬度随烧结温度的变化规律.结果表明,采用连续成型方式可使素坯密度提高56%、烧结时 间缩短了3h、致密化温度降低200℃.场发射扫描电镜显示烧结体内部密度及颗粒尺寸分布 均匀.硬度测定结果显示ZnO纳米块体材料中显微硬度随烧结温度的变化不是单调的,而是随 烧结温度的升高显微硬度先升高后降低,拐点对应的晶粒尺寸为50—60nm.关键词:ZnO纳米块体连续成型硬度  相似文献   

10.
反应溅射法制备TiO2薄膜   总被引:10,自引:0,他引:10  
赵坤  朱凤  王莉芳  孟铁军  张保澄  赵夔 《物理学报》2001,50(7):1390-1395
报道了用反应溅射法制备TiO2薄膜的实验研究.详细研究了氧分压、基底温度和退火温度对成膜结构的影响.制备出了具有金红石和锐钛矿晶体结构的TiO2薄膜.分析了金红石和锐钛矿晶体的形成条件,并对薄膜的表面形貌进行了测量.关键词:反应溅射2薄膜')\" href=\"#\">TiO2薄膜  相似文献   

11.
Transparent conducting zirconium-doped zinc oxide (ZnO:Zr) films were firstly deposited on polyethylene terephthalate (PET) substrates with ZnO buffer layers by DC magnetron sputtering at room temperature. Dependence of physical properties of ZnO:Zr films on deposition pressure was systematically studied. All the deposited films were polycrystalline and (1 0 0) oriented. When deposition pressure increases from 1 to 2.5 Pa, the crystallinity of the films improves and the resistivity decreases. While deposition pressure increases from 2.5 to 3.5 Pa, the crystallinity of the films deteriorates and the resistivity increases. The lowest resistivity of 1.8 × 10−3 Ω cm was obtained for the films deposited at the optimum deposition pressure of 2.5 Pa. All the films present a high transmittance of above 86% in the wavelength range of the visible spectrum.  相似文献   

12.
The nanocrystal thin films of zinc oxide doped by Al (ZnO:Al) were deposited by dc reactive magnetron sputtering on the glass substrates, in the pressure range of 33-51 Pa. From the X-ray diffraction patterns, the nanocrystalline structure of ZnO:Al films and the grain size were determined. The optical transmission spectra depend from the sputtering pressure, but their average value was 90% in the range from 33 Pa to 47 Pa. Also, the sputtering pressure changes the optical band gap of ZnO:Al films, which is highest for films deposited at 37 Pa, 40 Pa and 47 Pa. The obtained films at room temperature have a sheet resistance of 190 Ω/cm2 which increases with time, but the films annealed at temperature of 400 °C have constant resistance. The surface morphology of the films was studied by Scanning electron microscopy. XPS spectra showed that the peak of O1s of the as-deposited films is smaller than the peak of the annealed ZnO:Al films.  相似文献   

13.
Zinc oxide thin films were deposited by radio frequency magnetron sputtering at room temperature using a metallic zinc target in a gas mixture of argon and oxygen. Plasma power, oxygen /argon gas ratio, gas pressure, and substrate temperature were varied, and an experimental design method was used to optimize these deposition parameters by considering their interdependence. Crystalline structures and film stresses were examined. Post-deposition rapid thermal annealing was also carried out to observe its effects on the film properties. Statistical analysis was then used to find the optimal sputtering conditions. Results indicated that plasma power and gas pressure have the largest effects on film crystallization and stress and that postdeposition annealing can be used to improve the quality of the film properties.  相似文献   

14.
Thin films of zinc (Zn) were deposited onto glass substrates (maintained at room temperature) by thermal evaporation under vacuum. The metallic zinc films were submitted to thermal oxidation in air at 670 K and 770 K, respectively, for 5–90 min, in order to obtain zinc oxide (ZnO) thin films. X-ray diffraction patterns revealed that the ZnO thin films were polycrystalline and had a wurtzite (hexagonal) structure. The morphology of the prepared ZnO thin films was investigated using atomic force microscopy and scanning electron microscopy techniques. Transmission spectra were recorded in the spectral domain from 300 nm to 1400 nm. The optical energy bandgap calculated from the absorption spectra (supposing allowed direct transitions) was in the range 3.05–3.30 eV.  相似文献   

15.
The investigation of structure, optical and electrical properties of tin and zinc oxide films on glass substrates by using magnetron sputtering are carried out. X-ray data show the formation of textured tin oxides film during deposition and its transformation to SnO2 polycrystalline film at low temperature (200 C) if the concentration of oxygen in the chamber is high (O2 — 100%, Ar — 0%). Optimal conditions of SnO2 polycrystalline film deposition (pressure of Ar–O2 mixture in chamber — 2.7 Pa, concentration of O2 — 10%) are determined. Low resistivity of as-deposited ZnO film and increasing ZnO crystallite sizes and phase volume at temperatures higher than the melting point of Zn (419.5 C) are explained by formation of conductive Zn and ZnO particle chains and their destruction, respectively.  相似文献   

16.
反应磁控溅射法制备的氟化类金刚石薄膜的XPS结构研究   总被引:2,自引:0,他引:2  
江美福  宁兆元 《物理学报》2004,53(9):3220-3224
采用射频反应磁控溅射法用高纯石墨作靶、三氟甲烷(CHF3)和氩气(Ar)作源气体制 备了氟化类金刚石(FDLC)薄膜,通过XPS光谱结合拉曼光谱、红外透射光谱和紫外 可见光光谱研究了源气体流量比等工艺条件对薄膜中键结构、sp2/sp3杂化比以及光学带隙等性能的影响.结果表明在低功率(60W)、高气压(2.0Pa)和适当的流量比(Ar/CHF3=2∶ 1)下利用射频反应磁控溅射法可制备出氟含量高且具有较宽光学带隙和超低介电常数的FDLC薄膜.关键词:反应磁控溅射氟化类金刚石薄膜红外透射光谱XPS光谱  相似文献   

17.
王欣  高丽娟  于陕升  郑伟涛  徐娓  郭巍  杨开宇 《发光学报》2003,24(4):431-434,T002
利用直流磁控溅射方法,以Ar/N2作为放电气体,通过改变放电气体中N2的流量(N2流量比分别为5%,10%,30%,50%)及溅射时间(160,30,20,10,5min),在玻璃衬底上沉积了FexN薄膜。用X射线光电子能谱(XPS)方法确定了不同N2流量下薄膜的成分;X射线衍射(XRD)方法分析了不同N2流量下的FexN薄膜结构,当N2流量比为5%时获得了FeN0 056相,10%时为ε Fe3N相,30%和50%流量比下均得到FeN相。利用原子力显微镜(AFM)和掠入射X射线散射(GIXA)方法研究了膜表面的粗糙度和形貌,发现随着N2流量的增加,薄膜表面光滑度增加,薄膜表面呈现自仿射性质。动力学标度方法定量分析表明:薄膜表面因不同N2流量的影响而具有不同的动力学指数,当氮气流量比为5%时,静态标度指数α≈0 65,生长指数β≈0 53±0 02,薄膜生长符合基于Kolmogorov提出的能量波动概念的KPZ模型指数规律。  相似文献   

18.
氟化类金刚石薄膜的拉曼和红外光谱结构研究   总被引:4,自引:0,他引:4  
江美福  宁兆元 《物理学报》2004,53(5):1588-1593
关键词:  相似文献   

19.
Zinc oxide films with c-axis preferred orientation were deposited on silicon (100) substrates by radio frequency (RF) reactive sputtering. The properties of the sam- ples were characterized by X-ray diffractometer, X-ray photoelectron spectroscopy and fluorescent-spectrophotometer. The effect of sputtering power and substrate temperature on the structural and photoluminescent (PL) properties of the ZnO films was investigated. The results indicated that when the sputtering power is 100 W and the substrate temperature is 300-400℃, it is suitable for the growth of high c-axis orientation and small strain ZnO films. A violet peak at about 380 nm and a blue band at about 430 nm were observed in the room temperature photolumines- cence spectra, and the origin of blue emission was investigated.  相似文献   

20.
    
The effect of a magnetic field generated by a planar magnetron on the ion current distribution on the substrate has been investigated as a function of the substrate voltage and gas pressure for two configurations of the magnetic field. The probe and the substrate were biased by negative potentials of −60 to −280 V with respect to the grounded anode, in order to collect the saturated ion current and investigate the influence of the magnetron magnetic field on the distribution of the ion flux of the vacuum arc source. It was shown that the planar magnetron placed under the substrate strongly affects the ion current and ion current distribution near the substrate. For a broad pressure range, the maximum ion flux collected by the probe increased by 40%, while the net ion current to the substrate increased by 20%. We have demonstrated that the ion current increased by 18%, and maximum ion current density increased by 40%. The results were explained in terms of the plasma flux interaction with the magnetic field of the magnetron. The setup may be suitable for controlling ion flux density on large substrates.

  相似文献   


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