非晶硅碳(a-SiC:H)薄膜光学常数的透射谱表征

报道了一种用透射谱数据分析法计算非晶硅碳薄膜的厚度、折射率、吸收系数和光学带隙等光学常数的方法和程序.这一方法引用有效谐振子模型理论的折射率色散关系,所有公式均为解析表达式,便于进行数据处理,无须专用软件,使用Excel即可完成,适用于多种半导体薄膜材料.将这种方法应用于PECVD方法制备的非晶硅碳(a-SiC∶H)薄膜,对其光学特性进行了分析.     

非晶硅碳（a-SiC∶H）薄膜光学常数的透射谱表征

报道了一种用透射谱数据分析法计算非晶硅碳薄膜的厚度、折射率、吸收系数和光学带隙等光学常数的方法和程序．这一方法引用有效谐振子模型理论的折射率色散关系，所有公式均为解析表达式，便于进行数据处理，无须专用软件，使用Excel即可完成，适用于多种半导体薄膜材料．将这种方法应用于PECVD方法制备的非晶硅碳（a-SiC∶H）薄膜，对其光学特性进行了分析．     

玻璃上热壁真空沉积生长CdTe薄膜的结构及光学特性

采用热壁真空沉积的方法,在清洁的玻璃衬底上生长了不同膜厚的CdTe薄膜,对其结构和薄膜的本征吸收光学特性进行了测量分析研究.XRD测试显示薄膜为多晶,具有标准的立方结构,沿(111)方向有明显的择优取向.晶格常数的计算值为0.649nm,与标准值符合得较好.用Cary 5000型双光束分光光度计测试了薄膜的反射谱和透射谱,显示在本征吸收区透过率随着膜厚的增加和波长的减小而减小.对测量的反射谱和透射谱采用较严格的数学处理,计算得到了描述薄膜宏观光学特性的重要物理量,即薄膜的吸收系数、消光系数、折射率等.用(hvα)2对hv作图,得出了薄膜厚度为0.12,0.48和0.81μm的光学能隙分别为1.54,1.48和1.46eV,证实了材料是直接带隙结构,且在本征吸收的可见光区有高的吸收系数.     

玻璃上热壁真空沉积生长CdTe薄膜的结构及光学特性

采用热壁真空沉积的方法,在清洁的玻璃衬底上生长了不同膜厚的CdTe薄膜,对其结构和薄膜的本征吸收光学特性进行了测量分析研究.XRD测试显示薄膜为多晶,具有标准的立方结构,沿(111)方向有明显的择优取向.晶格常数的计算值为0.649nm,与标准值符合得较好.用Cary 5000型双光束分光光度计测试了薄膜的反射谱和透射谱,显示在本征吸收区透过率随着膜厚的增加和波长的减小而减小.对测量的反射谱和透射谱采用较严格的数学处理,计算得到了描述薄膜宏观光学特性的重要物理量,即薄膜的吸收系数、消光系数、折射率等.用(hvα)2对hv作图,得出了薄膜厚度为0.12,0.48和0.81μm的光学能隙分别为1.54,1.48和1.46eV,证实了材料是直接带隙结构,且在本征吸收的可见光区有高的吸收系数.     

有机半导体薄膜的光学和电学性质研究

采用真空热蒸镀技术制备了NPB有机半导体薄膜和单层夹心结构器件,通过透射谱测量研究了薄膜的光学能隙、折射率和消光系数等光学性质,结果表明有机半导体薄膜具有直接带隙半导体的光学性质,并且其折射率色散性质遵循单振子模型.另外,通过分析器件的电流-电压特性研究了薄膜的电导率、载流子迁移率和载流子浓度等电学性质.这些实验结果对于有机光电子器件的结构设计具有一定的参考价值.     

非晶态锑化铟薄膜的射频磁控溅射生长及其结构和光学特性研究

在玻璃衬底上用射频磁控溅射技术进行了非晶态锑化铟(a-InSb)薄膜的低温生长.采用X射线衍射(XRD)和原子力显微(AFM)技术对所生长的薄膜进行分析研究,所生长的非晶态锑化铟薄膜表面平整,没有晶粒出现,获得了射频磁控溅射生长非晶态锑化铟薄膜的"生长窗口".采用傅立叶红外透射光谱分析技术对非晶态锑化铟薄膜进行了光学性能研究,在0.9～2.0μm范围内研究了薄膜的透射谱线,获得了薄膜的吸收系数,研究了其光学带隙和吸收边附近的3个吸收区域.     

非晶态碲镉汞薄膜的射频磁控溅射生长及其结构和光学特性

在玻璃衬底上用射频磁控溅射技术进行了非晶态碲镉汞(α-HgCdTe,α-MCT)薄膜的低温生长.采用X射线衍射(XRD)和原子力显微(AFM)技术对所生长的薄膜进行分析研究,所生长的非晶态HgCdTe薄膜表面平整,没有晶粒出现,获得了射频磁控溅射生长非晶态HgCdTe薄膜的"生长窗口".采用傅里叶红外透射光谱分析技术对非晶态HgCdTe薄膜进行了光学性能研究,在1.0～2.0μm范围内研究了薄膜的透射谱线,获得了薄膜的吸收系数(～8×104cm-1),研究了其光学带隙(约0.83eV)和吸收边附近的3个吸收区域.     

非晶态碲镉汞薄膜的射频磁控溅射生长及其结构和光学特性

在玻璃衬底上用射频磁控溅射技术进行了非晶态碲镉汞(α-HgCdTe,α-MCT)薄膜的低温生长.采用X射线衍射(XRD)和原子力显微(AFM)技术对所生长的薄膜进行分析研究,所生长的非晶态HgCdTe薄膜表面平整,没有晶粒出现,获得了射频磁控溅射生长非晶态HgCdTe薄膜的"生长窗口".采用傅里叶红外透射光谱分析技术对非晶态HgCdTe薄膜进行了光学性能研究,在1.0～2.0μm范围内研究了薄膜的透射谱线,获得了薄膜的吸收系数(～8×104cm-1),研究了其光学带隙(约0.83eV)和吸收边附近的3个吸收区域.     

Pb1-xMnxTe稀磁半导体外延薄膜的光学特性

采用分子束外延(MBE)方法在BaF2(111)衬底上生长了不同Mn组分的Pb1-xMnxTe(0≤x≤0.012)稀磁半导体薄膜.通过波长为3.0~11.0μm中红外透射谱的分析并应用透射光谱上干涉峰峰值的位置计算获得了Pb1-xMnxTe薄膜的折射率,由最小平方根拟合得到折射率的一阶Sellmeier色散关系.在吸收边附近,通过直接跃迁吸收系数与光子能量的关系外推得到其光学带隙.结果表明,在中红外区域其折射率随着Mn含量的增加而减小,其光学带隙则随着Mn含量的增加而增大,在温度T=295K时,随着Mn含量x由0变化到0.012,其光学带隙Eg由0.320eV增加到0.370eV.     

硒化温度对SnSe2薄膜材料性能的影响

采用射频磁控溅射加硒化的两步法在超白玻璃衬底上生长SnSe₂薄膜,采用XRD、光学透过谱、Raman光谱、XPS和SEM等方法对薄膜进行性能表征。通过设置不同的硒化温度,研究不同硒化温度对所得薄膜相结构、物相与组分、表面形貌等性能的影响。结果表明:350℃,40min硒化所得薄膜为片状晶粒,光学带隙为1.46eV,相结构和均匀性等性能在该硒化条件下均为最佳。     

纳米硅薄膜光学性质的测定与研究

通过测定纳米硅薄膜的透射谱,建立计算模型计算得出薄膜样品的折射率、厚度、吸收系数和光能隙.计算结果表明这种半导体材料在620 nm波长附近的折射率约为3.4,计算得到的厚度与用台阶仪测量的结果吻合很好.在620 nm波长附近的吸收系数介于吸收系数较小的晶体硅与吸收系数较大的非晶硅之间,光能隙约为1.6 eV,两者都随晶态含量增大而呈减小趋势.     

镧掺杂BiGaO3多晶薄膜光学性质

采用溶胶-凝胶技术在Pt/Ti/SiO_2/Si衬底上制备了不同镧掺杂浓度BiGaO_3(Lx BGO,0≤x≤0.1)薄膜.X-射线衍射(XRD)表明该属于正交晶系的多晶薄膜,原子力显微镜(AFM)图像显示样品表面具有很好的平整性.采用椭圆偏振技术对其光学性质进行了详细的研究,发现其光学常数符合Adachi色散模型.进一步发现其禁带宽度随着镧掺杂浓度的增加而增加,该规律与理论预言相吻合.有关LxBGO材料的研究为铋基光电器件如紫外探测器的实现提供物理基础支持.     

衬底温度和氮气分压对氮化锌薄膜的性能影响

采用射频磁控溅射法在不同衬底温度和不同氮气分压下在石英玻璃衬底上制备氮化锌薄膜. 利用XRD和喇曼散射仪分析了样品的晶体结构和组成. 结果表明当氮气分压为1/2时可以生成多晶单一相的氮化锌薄膜. 利用霍尔效应和光学透过谱测量了样品的电学和光学性质. 结果表明衬底温度对样品的电学和光学性质有很大的影响. 衬底温度从100℃上升到300℃时,样品的电阻率从0.49降低到0.023Ω·cm. 电子浓度从2.7×1016升高到8.2×1019cm-3. 在衬底温度为200℃,氮气分压为1/2时,样品的光学带隙为1.23eV.     

Structural, electrical and optical characterization of semiconducting Ru2Si3

Recent band structure calculations indicate, that ruthenium silicide (Ru₂Si₃) is semiconducting with a direct band gap. Electrical measurements lead to a band gap around 0.8 eV which is technologically important for fiber communications. This makes Ru₂Si₃ a promising candidate for silicon-based optical devices, namely LEDs. We present results on the epitaxial growth of ruthenium silicide films on Si(100) and Si(111) fabricated by the template method, a special molecular beam epitaxy technique. We structurally characterized the films by Rutherford backscattering and ion channeling, X-ray diffraction and transmission electron microscopy. To determine the electrical resistivity at high temperatures films were grown on insulating substrates to prevent parallel conduction through the substrate. Finally we show first results of the optical absorption performed by photothermal deflection spectroscopy indicating pronounced absorption above 1.5 eV.     

Structural and optical properties of Zn-doped β-Ga_2O_3 films

正Intrinsicβ-Ga_2O_3 and Zn-dopedβ-Ga_2O_3 films were prepared using RF magnetron sputtering.The effects of the Zn doping and thermal annealing on the structural and optical properties are investigated.In comparison with the intrinsicβ-Ga_2O_3 films,the microstructure,optical transmittance,optical absorption,optical energy gap,and photoluminescence of Zn-dopedβ-Ga_2O_3 films change significantly.The post-annealedβ-Ga_2O_3 films are polycrystalline.After Zn doping,the crystallization deteriorates,the optical band gap shrinks,the transmittance decreases and the UV,blue,and green emission bands are enhanced.     

Optical Constants and Structure of ZnO Films by Radio Frequency Magnetron Sputtering

ZnO films are deposited on glass slides by radio frequency（RF） magnetron sputtering under different powers. The polycrystal structures and surface morphologies of the film are investigated. The optical transmission spectra for the ZnO films are measured within the range from 300 nm to 800 nm. The optical constants and thickness of the films are determined using a nonlinear programming method suggested by Birgin et al. The band gap of the film increases with reducing the nano-size of the film grains. The packing density of the films can be improved by reducing the RF power.     

热致漂白效应对非晶Ge34Ga2S64薄膜结构和光学特性的影响

采用热蒸发法技术沉积Ge34Ga2S64非晶薄膜,并对薄膜样品在375℃热处理2h。通过分光光度计、表面轮廓仪和显微拉曼光谱仪测试热处理前后薄膜样品的透过曲线、薄膜厚度和拉曼结构。利用薄膜干涉曲线的波峰和波谷计算了薄膜的厚度和折射率,并根据Swanepoel方法以及Tauc公式分别计算了薄膜折射率色散曲线和光学带隙等参数。结果表明,Ge34Ga2S64非晶薄膜经热处理后发生热致漂白效应,大分子团簇以及Ge-Ge、S-S同极错键含量明显减少,网络结构无序性降低,从而引起薄膜的光学吸收边蓝移、折射率降低、表面粗糙度(Ra)降低0.515nm和光学带隙增大0.118eV。     

The optical band gap of hydrogenated amorphous boron thin films: The effect of substrate temperature

Hydrogenated amorphous boron thin films have been produced on quartz substrates heated to 150, 250, and 350°C by the glow discharge decomposition of a gas mixture of 5 v/o BoHg and 95 v/o H₂. Doped films have also been prepared by the addition of 1 a/o C₂H₄ or 0.5 a/o SiH₄. The absorp-tion coefficients as a function of wavelength across the visible spectrum and the concomitant optical band gaps of all films were measured. The optical band gaps of the films produced at 150 and 250°C were approximately 2.1 eV while those films produced at 350°C showed band gaps between 1.6 and 1.4 eV. These results indicate that it is possible to optimize theroretical photovoltaic conversion efficiencies of solar cells based on hydrogenated amorphous boron thin films produced by glow discharge methods through the tailor-ing of the optical band gap by control of substrate temper-ature.     

Band gap widening and narrowing in moderately and heavily doped n-ZnO films

In semiconductors, a widening of the optical band gap occurs because the lower states in the conduction band are blocked. At the same time band gap narrowing also occurs due to many body interactions on doping. This paper reports the analysis of widening and narrowing of optical band gap in sol–gel derived ZnO films moderately doped with Yttrium and heavily doped sputtered ZnO films with aluminum and scandium. The band gap was evaluated using optical transmission data. Carrier concentration was known from the Hall measurements. At high concentrations the effective change in band gap is found to be the difference of the band gap widening and band gap narrowing. At low concentration of dopant the many body theories do not apply and the experiments also show that the band gap narrowing is practically negligible at these concentrations and the effective band gap widening is determined by the band gap widening alone. The chemical nature of the dopant played practically no role.     

AlN外延薄膜的生长和特征

文章研究了AlN薄膜的晶体质量、表面形貌、应力等性质与AlN生长工艺的依赖关系。通过对低温成核厚度、成核温度和高温生长AlN所用Ⅴ／Ⅲ比的研究，制备出了具有较好晶体质量的AlN薄膜。高分辨三晶X射线衍射给出AlN薄膜的(002)和(105)的半高宽分别为16．9arcsec和615arcsec，接近国际上报道的较好结果。原子力显微镜对表面形貌的分析表明AlN薄膜的粗糙度为5．7nm。拉曼光谱表明E2(high)模向高能方向移动，说明蓝宝石上外延的AlN薄膜处于压应变状态。光学吸收谱在204nm处具有陡峭的带边吸收，也表明了AlN外延薄膜具有较好地晶体质量。