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1.
反应淀积氮化铝薄膜及其性质的研究   总被引:9,自引:0,他引:9  
实验使用脉冲激光熔蚀金属铝靶,使溅射的物质粒子和真空室中的氮气反应以淀积氮化铝(AlN)薄膜,淀积时引入氮气直流放电以促使Al和N发生完全反应制备高质量符合化学计量比的AlN薄膜。讨论了脉冲能量密度、基底温度、气体放电对所沉积薄膜组织结构的影响。实验结果表明,当DE=1.0J·cm-2,PN2=13.333kPa,Tsub=200℃,V=650V,f=5Hz,dS-T=4cm时,高质量的AlN薄膜被成功地沉积于Si(100)基片上。分析表明薄膜是具有高取向性的AlN(100)多晶膜,薄膜的能带间隙约为6.2eV,其电阻率和击穿电场分别为2×1013Ω·cm和3×106V·cm-1。  相似文献   

2.
用PECVD法在金属衬底上沉积氮化硅薄膜   总被引:2,自引:0,他引:2  
采用等离子体增强化学气相沉积(PECVD)方法在40Cr钢(含Cr0.8%~1.1%)或铜等金属基片上沉积氨化硅薄膜。沉积温度为250℃时,制备的薄膜厚度为0.2~0.4μm,电阻率为8×10 ̄(16)Ω·cm,介质击穿场强达到1×10 ̄7V/cm。用XPS谱研究了薄膜的结构和成分,并分析了沉积时不同的工艺参数对薄膜绝缘耐压性能的影响。  相似文献   

3.
蒋美萍  黄宜平 《微电子学》1996,26(3):156-159
用机械减薄和氧化剥层法获得表层硅厚度约0.4μm的BESOI薄膜。对这种薄膜用Secco腐蚀液腐蚀并分析了缺陷种类,计量了缺陷密度。用波长为0.5145μm的激光Raman谱测量了BESOI薄膜和界面附近的应力密度。结果表明,该薄膜的主要缺陷为氧化层错,密度约1.8×103/cm2,总的缺陷密度为2.6×103/cm2,张应力密度δ≤5×103N/cm2。  相似文献   

4.
多元多色HgCdTe红外探测器   总被引:2,自引:2,他引:0  
简要介绍利用不同波段的微型滤光片和不同响应波段的多元HgCdTe红外探测器,叙述了通过精密镶嵌技术组合而成的四波段215~225μm、84~89μm、103~113μm和115~125μm88元多元多色探测器的设计原理和特性,以及多元多色探测器的组合工艺,并给出了各个通道的响应光谱特性和探测器的工作性能。研制成功的88元多色红外探测器每个通道的平均探测率和响应率分别为:D2.15~2.25=1.2×1012cmHz1/2/W和R2.15~2.25=5.0×106V/W,D8.4~8.9=7.0×1010cmHz1/2/W和R8.4~8.9=1.6×104V/W,D10.3~11.3=4.0×1010cmHz1/2/W和R10.3~11.3=4.3×103V/W,D11.5~12.5=3.0×1010cmHz1/2/W和R11.5~12.5=3.3×103V/W,文中对这些结果进行了分析和讨论。  相似文献   

5.
0.15μm薄膜全耗尽MOS/SOI器件的设计和研制   总被引:6,自引:6,他引:0  
张兴  王阳元 《半导体学报》2000,21(2):156-160
利用自己开发的二维数值深亚微米SOI器件模拟软件,较为详细地分析了沟道长度小于0.2μm的SOI器件的阈值电压特性、穿通和击穿特性、亚阈值特性以及直流稳态特性等.通过这些模拟和分析计算,给出了沟道长度为0.18、0.15和0.1μm的薄膜全耗尽SOI/MOS器件的设计方案,并根据该设计方案成功地研制出了性能良好的沟道长度为0.15μm的凹陷沟道SOI器件.沟道长度为0.15μm薄膜全耗尽凹陷沟道SOI器件的亚阈值斜率为87mV/dec,击穿电压为1.6V,阈值电压为0.42V,电源电压为1.5V时的驱动电  相似文献   

6.
CdTe/ZnS复合钝化膜的界面电学特性研究   总被引:1,自引:0,他引:1  
利用MIS结构研究了长、中、短波碲镉汞材料,新型热蒸发CdTe/ZnS钝化膜界面电学特性及其与工艺条件的关系.结果表明,CdTe/ZnS双层膜界面电学参数依赖于界面预处理条件,在适当的工艺条件下,平带电压几乎为0,固定电荷密度为-4×1010cm-2,慢态密度为5.1×1010cm-2,界面态密度为2.7×10-11eV-1.cm-2.  相似文献   

7.
文中报导了用分子束外廷工艺在GaAs(211)B衬底上生长了较高质量的中、长波HgCdTe薄膜材料。生长后的材料通过退火进行转型和调节电性参数。选择的组分分别为x=0.330和0.226的两种材料,77K时载流子浓度和迁移率分别为p=6.7×1015cm-3、up=260cm2V-1s-1和4.45×1015cm-3、410cm2V-1s-1。研制了平面型中、长波线列光伏探测器,其典型的探测器D分别为5.0×1010cmHz1/2W-1和2.68×1010cmHz1/2W-1(180°视场下),其中64元线列中波探测器与CMOS电路芯片在杜瓦瓶中耦含后读出并实现了红外成像演示。  相似文献   

8.
在氮气气氛中用石墨电弧法合成了氮掺杂富勒烯.质谱、紫外、红外分析等手段证实了样品中含有C59N、C59N2、C59N4、C59N6以及C70N2等分子团簇,对蒸发制备的薄膜进行3小时200℃退火测得其室温电导率为1e-6(S/cm),激活能为0.69eV(常温),0.56eV(高温).  相似文献   

9.
氢化非晶硅带隙态密度光诱导变化的研究   总被引:1,自引:1,他引:0  
报导了与Staebler-Wronski效应相关的氢化非晶硅(α-Si:H)带隙态密度的光诱导变化,结果表明光照将使α-Si:H带隙上半部分态密度的分布发生变化,采用AM1太阳光谱*光照两小时使得导带迁移率边以下0.7eV处的带隙态密度从4×1016cm-3eV-1,增大到1×1017cm-3eV-1。  相似文献   

10.
采用计算机控制的快速辐射加热、超低压CVD(RRH/VLP-CVD)方法生长了Si/Si0.7Ge0.3/Sip-型调制掺杂双异质结构.研究了该结构的输运性质,其空穴霍尔迁移率高达300cm2/V·s(300K,薄层载流于浓度ps为2.6e13cm-2)和8400cm2/V·s(77K,ps为1.1e13cm-2).  相似文献   

11.
A detailed theoretical study of the electronic structure, optical, elastic and thermodynamics properties of jadeite have been performed by means of the first principles based on the state-of-the-art of density functional theory within the generalized gradient approximation. The optimized lattice constants and the atomic positions are in good agreement with experimental data. The total density of states and partial density of states of jadeite have been discussed. The energy gap has been calculated along the Γ direction found to be 5.338 eV, which shows that jadeite has wide direct band gap. The optical properties, such as the dielectric function, refractive index, extinction coefficient, reflectivity coefficient, loss function and absorption coefficient for [100] and [001] directions have been described for the first time in the energy range 0–40 eV. The elastic constants, bulk modulus, Young׳s modulus, anisotropic factor and Poisson׳s ratio have been calculated. Furthermore, the Vickers hardness and Debye temperature of jadeite have been predicted. The calculated values of all above parameters are compared with the available experimental values.  相似文献   

12.
The cubic BiGaO3 and BiInO3 perovskite oxides have been investigated for their structural stability, mechanical and opto-electronic properties by employing the density functional theory. The exchange-correlation effects have been modeled with Perdew–Burke–Ernzerhof generalized gradient approximation, while the improved evaluation of electronic properties has been achieved by using the Tran–Blaha modified form of semi-local Becke–Johnson functional. Structural properties are calculated and the thermodynamics stability of BiGaO3 and BiInO3 in the cubic perovskite structure has been established in terms of enthalpies of formation. Furthermore, elastic coefficients such as Cij, bulk modules B, anisotropy factor, shear modulus G, Young’s modulus Y, Poisson’s ratio ν, and B/G ratio are predicted. Band structure calculations reveal that investigated compounds have an indirect band gap between the occupied O 2p and unoccupied Bi 6p orbitals. The optical response of BiGaO3 and BiInO3 are also inspected by computing the complex dielectric function, refractive index, absorption coefficient, extinction coefficient, reflectivity and optical conductivity for radiation with energy up to 16 eV. The important thermoelectric properties of the compounds are described in terms of thermal conductivity, electrical conductivity, Seebeck coefficient and figure of merit.  相似文献   

13.
为了提高 SnO_2-LiZnVO_4系湿敏材料的性能,采用共沉淀法制备出 SnO_2-K_2O-LiZnVO_4系纳米湿敏粉体。考察了液相掺杂 K+对材料湿敏性能、复阻抗特性和电容特性的影响。实验结果表明,采用共沉淀法制备纳米粉体并使K+液相掺杂量为 2.5%(摩尔分数),可使湿敏材料低湿电阻小、灵敏度适中,适当的 K+添加量可明显改善 SnO_2-LiZnVO_4系纳米材料的感湿特性。  相似文献   

14.
Nanocrystalline CdO thin films were prepared onto a glass substrate at substrate temperature of 300 °C by a spray pyrolysis technique. Grown films were annealed at 250, 350, 450 and 550 °C for 2.5 h and studied by the X-ray diffraction, Hall voltage measurement, UV-spectroscopy, and scanning electron microscope. The X-ray diffraction study confirms the cubic structure of as-deposited and annealed films. The grain size increases whereas the dislocation density decreases with increasing annealing temperature. The Hall measurement confirms that CdO is an n-type semiconductor. The carrier density and mobility increase with increasing annealing temperature up to 450 °C. The temperature dependent dc resistivity of as-deposited film shows metallic behavior from room temperature to 370 K after which it is semiconducting in nature. The metallic behavior completely washed out by annealing the samples at different temperatures. Optical transmittance and band gap energy of the films are found to decrease with increasing annealing temperature and the highest transmittance is found in near infrared region. The refractive index and optical conductivity of the CdO thin films enhanced by annealing. Scanning electron microscopy confirms formation of nano-structured CdO thin films with clear grain boundary.  相似文献   

15.
We present a theoretical study of structural, elastic, thermodynamic, and electronic properties of the uranium filled skutterudite UFe4P12. We use the full-potential linear muffin–tin orbital (FP-LMTO) method in which the local density approximation (LDA) is used for the exchange-correlation (XC) potential. The lattice parameter at equilibrium, the bulk modulus, its pressure derivative, the elastic constants and the band structure energy of the filled skutterudite UFe4P12 are calculated and systematically compared to available theoretical and experimental data. Herein, we use the total energy variation as function of strain technique to determine independent elastic constants and their pressure dependence. Furthermore, using quasi-harmonic Debye model with phonon effects, the effect of pressure P and temperature T on the lattice parameter, bulk modulus, thermal expansion coefficient, Debye temperature and the heat capacity of UFe4P12 are investigated for the first time. Band structure of UFe4P12 indicates a tendency of forming a pseudo-gap that appears above the Fermi level at Γ point. This is a unique characteristic of skutterudite, especially when a single phosphorous p-band crosses the Fermi level. The crossing band is, indeed, pushed down by the repulsion of U f-resonance states.  相似文献   

16.
Manganese indium sulphide (MnIn2S4) thin films were deposited using an aqueous solution of MnCl2, InCl3 and (NH2)2CS in the molar ratio 1:2:4 by simple chemical spray pyrolysis technique. The thin film substrates were annealed in the temperature range between 250 and 350 °C to study their various physical properties. The structural properties as studied by X-ray diffraction showed that MnIn2S4 thin films have cubic spinel structure. The formation of cube and needle shaped grains was clearly observed from FE-SEM analysis. The energy dispersive spectrum (EDS) predicts the presence of Mn, In and S in the synthesized thin film. From the optical studies, it is analyzed that the maximum absorption co-efficient is in the order between 104 and 105 cm−1 and the maximum transmittance (75%) was noted in the visible and infrared regions. It is noted that, the band gap energy decreases (from 3.20 to 2.77 eV) with an increase of substrate temperature (from 250 to 350 °C). The observations from photoluminescence studies confirm the emission of blue, green, yellow and red bands which corresponds to the wavelength range 370–680 nm. Moreover, from the electrical studies, it is observed that, as the substrate temperature increases the conductivity also increases in the range 0.29–0.41×10−4 Ω−1 m−1. This confirms the highly semiconducting nature of the film. The thickness of the films was also measured and the values ranged between 537 nm (250 °C) to 483 nm (350 °C). This indicates that, as the substrate temperature increases, the thickness of the film decreases. From the present study, it is reported that the MnIn2S4 thin films are polycrystalline in nature and can be used as a suitable ternary semiconductor material for photovoltaic applications.  相似文献   

17.
Structural, electrical, and optical properties of undoped and Zn doped lead sulfide (PbS) thin films are benign reported in this paper. The subjected films were grown on glass substrates at 25 °C by a chemical bath deposition (CBD) method. The concentration of Zn in the deposition bath represented by the ratio [Zn2+]/[Pb2+] was varied from 0% to 5%. It was found that the film׳s grains decreased in size with increasing Zn content in the film. XRD data showed the polycrystalline nature of the film its crystal orientation peak intensities decreased with higher doping concentration of Zn. Atomic force microscopy (AFM) measurements revealed that the surface roughness of the films decreased due to zinc doping as well. However, with increasing of the dopant concentration from 0% to 5%, the average transmittance of the films varied over the range of 35–75%. The estimated optical band (Eg) gaps of undoped and Zn doped PbS thin films were in the range of 0.72–1.46 eV. Hall Effect measurements electrical resistivity, carrier concentration and Hall mobility have been determined for the titled film as functions on the Zn content within the film׳s textures. The overall result of this work suggested that the Zn:PbS film is a good candidate as an absorber layer in the modern solar cell devices.  相似文献   

18.
Effect of rhenium doping is examined in single crystals of MoSe2 viz. MoRe0.005Se1.995, MoRe0.001Se1.999 and Mo0.995Re0.005Se2, which is grown by using the direct vapor transport (DVT) technique. The grown crystals are structurally characterized by X-ray diffraction, by determining their lattice parameters a and c, and X-ray density. Also, the Hall effect and thermoelectric power (TEP) measurements show that the single crystals exhibit a p-type semiconducting nature. The direct and indirect band gap measurements are also undertaken on these semiconducting materials.  相似文献   

19.
正Effect of rhenium doping is examined in single crystals of MoSe_2 viz.MoRe_(0.005)Se_(1.995), MoRe_(0.001)Se_(1.999) and Mo_(0.995)Re_(0.005)Se_2,which is grown by using the direct vapor transport(DVT) technique. The grown crystals are structurally characterized by X-ray diffraction,by determining their lattice parameters a and c,and X-ray density.Also,the Hall effect and thermoelectric power(TEP) measurements show that the single crystals exhibit a p-type semiconducting nature.The direct and indirect band gap measurements are also undertaken on these semiconducting materials.  相似文献   

20.
Nanocrystalline Zn1-x CoxO(where x varies from 0 to 0.04 in steps of 0.01) thin films were deposited onto glass substrate by the spray pyrolysis technique at a substrate temperature of 350 ℃. The X-ray diffraction patterns confirm the formation of hexagonal wurtzite structure. The crystal grain size of these films was found to be in the range of 11–36 nm. The scanning electron micrographs show a highly crystalline nanostructure with different morphologies including rope-like morphology for undoped ZnO and nanowalls and semispherical morphology for Co-doped Zn O. The transmittance increases with increasing Co doping. The optical absorption edge is observed in the transmittance spectra from 530 to 692 nm, which is due to the Co2C absorption bands corresponding to intraionic d–d shifts. The direct and indirect optical band gap energies decrease from 3.05 to 2.75 eV and 3.18 to 3.00 eV, respectively for 4 mol% Co doping. The electrical conductivity increases with increasing both the Co doping and temperature, indicating the semiconducting nature of these films. The temperature dependence thermal electromotive force measurement indicates that both undoped and Co-doped ZnO thin films show p-type semiconducting behavior near room temperature. This behavior dies out beyond 313 K and they become n-type semiconductors.  相似文献   

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