不同衬底上纳米晶CdTe薄膜的低温制备及光性能研究

CdTe nanocrystalline thin films have been prepared on glass, Si and Al2O3 substrates by radio-frequency magnetron sputtering at liquid nitrogen temperature. The crystal structure and morphology of the films were charac-terized by X-ray diffraction （XRD） and field-emission scanning electron microscopy （FESEM）. The XRD examinations revealed that CdTe films on glass and Si had a better crystal quality and higher preferential orientation along the （111） plane than the Al2O3. FESEM observations revealed a continuous and dense morphology of CdTe films on glass and Si substrates. Optical properties of nanocrystalline CdTe films deposited on glass substrates for different deposited times were studied.     

射频磁控溅射法低温沉积MnZn铁氧体薄膜

采用磁控溅射法在Si(100)、Si(111)和玻璃基片上原位沉积MnZn铁氧体薄膜,用X线衍射(XRD)仪、场发射扫描电子显微镜(FESEM)表征薄膜的物相结构与微观形貌,用振动样品磁强计(VSM)测试薄膜的磁性能.结果表明,在Si(100)基片上原位沉积的MnZn铁氧体薄膜,在较低的基片加热温度(Ts=50℃)下即可晶化;Ts升高,MnZn铁氧体薄膜的XRD衍射峰强度逐渐增强;当Ts≤150℃时,MnZn铁氧体薄膜X线衍射主峰为(311),但当Ts≥200℃后,MnZn铁氧体薄膜沿{111}晶面生长.在Si(111)和玻璃基片上沉积的MnZn铁氧体薄膜,其XRD衍射主峰分别为(111)和(311).     

Structural and electrical investigation of BLT films deposited at different times using electron beam evaporation technique

Thin films Bi4Ti3O12 (BLT) were deposited using electron beam evaporation on silicon substrate at several times, also on AlN/Si and SiO2/Si substrates. Thin films morphology and thickness were measured via scanning electron microscopy (SEM). The crystallography was studied using X-ray diffraction (XRD) technique for films which have a (0010) preferred orientation in all substrate types. The capacitance values were contingent on frequency value in C-V measurement. The ferroelectric characterization was investigated for BLT film deposited on isolator layer (SiO2 or AlN) for Al/Bi4Ti3O12/SiO2/Si devices. Memory effect value varied from 1 V to 3 V depending on the thin films isolator on substrate.     

溅射功率对AlN薄膜结构形貌的影响

采用直流反应磁控溅射法在Si(111)基片上制备了AlN薄膜,利用X线衍射(XRD)、场发射扫描电子显微镜(FESEM)、原子力显微镜(AFM)对不同溅射功率下制备的AlN薄膜的结构及形貌进行了分析表征。结果表明:在一定范围内,随着溅射功率的增大,薄膜厚度增加,晶粒逐渐长大,表面粗糙度也随之增大;AlN(002)择优取向改善明显,120W时达到最佳。     

Al_2O_3过渡层厚度对AZO薄膜性能的影响研究

采用磁控溅射法,在预先沉积了Al2O3过渡层的玻璃衬底上制备了性能优良的AZO薄膜。借助XRD、AFM、四探针仪和分光光度计对AZO薄膜的结构、表面形貌以及电学和光学性质进行了表征,并研究了Al2O3过渡层厚度对AZO薄膜性能的影响。结果表明:Al2O3过渡层的添加对AZO薄膜的表面形貌有一定影响;AZO薄膜的结晶质量随着过渡层厚度的增加先上升后下降;AZO薄膜的电阻率因过渡层的添加而明显降低,特别是在AZO薄膜较薄时;在添加了1～3 nm厚的过渡层后,160 nm厚的AZO薄膜的电阻率下降了44%左右;AZO薄膜的可见光透射率和光学带隙基本不受过渡层影响。     

超声喷雾热解法制备TiO2薄膜

成功地利用超声喷雾热解法在玻璃衬底上制备了TiO2薄膜。Ti（SO4）2作为钛源,甲醇作为溶剂。利用超声波的雾化作用将反应物形成细小的雾滴,并喷射到预热的玻璃衬底上分解而形成稳定的TiO2薄膜。为获得致密均匀的薄膜,优化了反应物浓度、温度、沉积时间等参数。利用X射线衍射与原子力显微镜表征了薄膜的晶体结构与表面形貌。X射线结果表明薄膜为多晶锐钛矿结构TiO2薄膜,并在（101）方向呈现出择优趋势。     

溅射功率对Mg2Si薄膜制备的影响

采用射频磁控溅射系统,在Si(111)衬底上制备了不同溅射功率下的Mg2Si薄膜。通过X线衍射(XRD)和冷场发射电子显微镜镜(FESEM)对Mg2Si薄膜的晶体结构和表面形貌进行了表征,理论分析了Mg2Si薄膜在Si(111)衬底上的外延生长关系,得到了Mg2Si薄膜的外延生长特性。研究结果表明,在80～110 W的溅射功率范围内,Mg2Si薄膜具有Mg2Si(220)的外延择优生长特性,并且随着溅射功率的增加Mg2Si(220)衍射峰先增强后变弱,在100W功率下Mg2Si(220)衍射峰最强。     

衬底对V_2O_5薄膜微观结构的影响

在常温下,用sol-gel法在普通玻璃和单晶Si衬底上制备了V2O5薄膜,并将样品在空气中于500℃进行热处理。通过XRD和SEM对比分析了不同衬底上样品的微观结构,用分光光度计测试了玻璃衬底上样品在350~850nm的光学特性。结果表明:在玻璃和Si衬底上分别得到了β-V2O5和α-V2O5薄膜,两种样品的纯度高、相结构单一和结晶度好。β-V2O5薄膜的光学带隙Eg为2.33eV。     

氧化钒薄膜的制备及电致开关特性的研究

采用反应溅射法,室温下,在Cu/Ti/SiO2/Si衬底上制备了氧化钒(VOx)薄膜,并对薄膜进行450℃、30min的真空退火处理.采用X-射线衍射(XRD)、原子力显微镜(AFM)对薄膜的结晶取向和表面形貌进行了表征,通过半导体参数分析仪对薄膜的电开关特性进行测试,并利用导电原子力显微镜(CAFM)对VOx薄膜的导...     

衬底对钛酸铋铁电薄膜生长及性能的影响

采用溶胶–凝胶工艺在Si和Pt/Ti/SiO2/Si两种衬底上制备了Bi4Ti3O12铁电薄膜,研究了衬底对Bi4Ti3O12铁电薄膜生长及性能的影响。研究表明:Pt/Ti/SiO2/Si基Bi4Ti3O12薄膜的剩余极化较高但易出现焦绿石相,而Si基Bi4Ti3O12薄膜易于沿c轴取向生长,有利于改善铁电薄膜与硅衬底之间的界面特性,但8mC/cm2的剩余极化却比前者有所降低。     

硅基镓浓度对GaN晶体膜质量的影响

采用射频磁控溅射工艺在扩镓硅基上溅射Ga2O3薄膜，再氮化反应组装GaN晶体膜，并对其生长条件进行了研究。用傅里叶红外谱仪(FTIR)、X射线衍射(XRD)、扫描电镜(SEM)、选区电子衍射(SAED)和光致发光(PL)谱对样品进行结构、形貌和发光特性的分析。测试结果表明，采用此方法可得到六方纤锌矿结构的GaN晶体膜。镓浓度在影响膜层质量方面起着不可忽视的作用，随着扩镓浓度的增加，薄膜的晶化程度和发光特性明显提高。     

玻璃和聚酰亚胺衬底上磁控溅射沉积的ZnO:Al透明导电膜的结构、电学和光学性能(英文)

利用射频磁控溅射方法在玻璃和聚酰亚胺膜(PI)衬底上沉积了氧化铝质量分数为2%的掺铝氧化锌透明导电薄膜(ZnO∶Al)。系统地研究了不同衬底材料对薄膜的结构、电学以及光学性能的影响。分析表明,衬底材料对薄膜的结晶性和电学性能有较大的影响,对可见光透射率却影响不大。X射线衍射(XRD)分析得出所有的ZnO∶Al具有良好的c轴择优取向性,在可见光区(400～800nm)两种衬底上的薄膜都达到了85%的透射率。玻璃衬底上的薄膜呈现出更强的(002)衍射峰及相对更小的半峰全宽(FWHM),薄膜电阻率达到了2.352×10-4Ω.cm。电镜分析表明,相对于PI上的ZnO∶Al膜,玻璃上ZnO∶Al膜表面有更致密的微观结构及更大的晶粒尺寸。PI衬底上的ZnO∶Al膜也有相对较好的电、光学性能,其中电阻率达到了6.336×10-4Ω.cm,而且由于PI衬底柔性可弯曲,使得它适于在柔性太阳电池和柔性液晶显示中做窗口层材料及透明导电电极。玻璃上的ZnO∶Al膜则可应用在平板显示和太阳电池技术中。     

Photoelectrochemical (PEC) studies on Cd0.5Fe0.5Se nanocrystalline thin films deposited by a spray pyrolysis technique

Recently, nanostructured thin films have attracted the attention of researchers from several disciplines, due to their outstanding electronic and optical properties and potential applications in various optoelectronic devices. The ternary Cd_0.5Fe_0.5Se nanocrystalline thin films were deposited by a spray pyrolysis method onto glass, aluminium, copper and stainless steel substrates. The structural and morphological properties were studied by X-ray diffraction and scanning electron microscopy analysis. The XRD study revealed that, Cd_0.5Fe_0.5Se films are nanocrystalline in nature with hexagonal lattice. The optical absorption study showed that, the semiconductor Cd_0.5Fe_0.5Se thin film deposited on glass exhibits direct band gap energy of the order of 1.95 eV. The PEC study revealed that, Cd_0.5Fe_0.5Se thin films deposited on aluminium substrate exhibited maximum fill factor (FF) and efficiency (η) as compared to the films deposited on stainless steel and copper substrates.     

Al掺杂ZnO薄膜的XPS谱及电学性质研究

采用直流反应磁控溅射法在玻璃基底上用Zn(99.99%)掺杂Al(1.5%)靶制备出高质量的Al掺杂的ZnO(AZO)薄膜。用X射线光电子能谱仪对退火处理后的薄膜进行了成分和元素的价态分析,并用Van der Pauw方法对样品的电学特性进行了测量。实验结果表明,Zn和Al元素都以氧化态的形式存在,O元素主要是以晶格氧和吸附氧的形式存在。AZO薄膜的电学性质受退火温度和氧氩比的影响较大。随着退火温度的升高,电阻率减小,载流子浓度和迁移率增大。随着氧氩比的增大,电阻率增大,迁移率减小。因此可得到用直流反应磁控溅射法制备AZO薄膜的最佳氧氩比和退火温度分别为0.3/27和400℃,在此条件下制备出的薄膜电阻率可低至10-4Ω.cm,载流子浓度可达1020cm-3。     

无机sol-gel法制备二氧化钒薄膜的研究

采用无机sol-gel法,以分析纯V2O5为原料,在Si衬底、玻璃衬底上空气中加热制备了V2O5薄膜,在不同温度下真空退火,得到了具有择优取向的VO2薄膜。研究了其制备工艺和显微结构。结果表明:在玻璃衬底和硅衬底上薄膜的最佳真空退火工艺均为480℃/2h。所制备的VO2薄膜具有沿<110>晶向生长的择优取向。薄膜表面形貌良好,颗粒尺寸分布均匀。     

Mg2Si薄膜在Si(100)衬底上的外延生长研究

采用直流磁控溅射系统,在Si(100)衬底上制备了外延Mg2Si半导体薄膜。通过XRD和场发射扫描电子显微镜(FESEM)对Mg2Si薄膜的晶体结构和表面形貌进行表征,理论分析了Mg2Si薄膜的消光特性对Mg2Si薄膜外延取向的影响,得到了Mg2Si薄膜的外延取向特性。结果表明,在Si(100)衬底上,外延Mg2Si薄膜具有Mg2Si(220)的择优生长特性。     

衬底温度对Al2O3掺杂ZnO透明导电薄膜性能的影响

以纯度为99.9％的陶瓷靶(w(ZnO)=98％,w(Al2O3)=2％)为溅射靶材,采用射频磁控溅射法在玻璃衬底上沉积制备了Al2O3掺杂的ZnO(AZO)薄膜.采用X射线衍射(XRD)仪、扫描电子显微镜(SEM)、紫外可见光谱(UV-Vis)仪等仪器,对AZO薄膜的形貌结构、光电学性能进行了测试,从薄膜生长方式和缺...     

Selective CdTe Nanoheteroepitaxial Growth on Si(100) Substrates Using the Close-Spaced Sublimation Technique Without the Use of a Mask

The development of HgCdTe detectors requires high sensitivity, small pixel size, low defect density, long-term thermal-cycling reliability, and large-area substrates. CdTe bulk substrates were initially used for epitaxial growth of HgCdTe films. However, CdTe has a lattice mismatch with long-wavelength infrared (LWIR) and middle-wavelength infrared (MWIR) HgCdTe that results in detrimental dislocation densities above mid-10⁶ cm^?2. This work explores the use of CdTe/Si as a possible substrate for HgCdTe detectors. Although there is a 19% lattice mismatch between CdTe and Si, the nanoheteroepitaxy (NHE) technique makes it possible to grow CdTe on Si substrates with fewer defects at the CdTe/Si interface. In this work, Si(100) was patterned using photolithography and dry etching to create 500-nm to 1-μm pillars. CdTe was selectively deposited on the pillar surfaces using the close-spaced sublimation (CSS) technique. Scanning electron microscopy (SEM) was used to characterize the CdTe selective growth and grain morphology, and transmission electron microscopy (TEM) was used to analyze the structure and quality of the grains. CdTe selectivity was achieved for most of the substrate and source temperatures used in this study. The ability to selectively deposit CdTe on patterned Si(100) substrates without the use of a mask or seed layer has not been observed before using the CSS technique. The results from this study confirm that CSS has the potential to be an effective and low-cost technique for selective nanoheteroepitaxial growth of CdTe films on Si(100) substrates for infrared detector applications.     

锡掺杂对碲化镉多晶薄膜形貌和光学性能的影响

Sn-doped CdTe polycrystalline films were successfully deposited on ITO glass substrates by close space sublimation. The effects of Sn-doping on the microstructure, surface morphology, and optical properties of polycrys- talline films were studied using X-ray diffraction, scanning electron microscopy, and ultraviolet-visible spectrophotometry, respectively. The results show that the lower molar ratio of Sn and CdTe conduces to a strongly preferential orientation of （111） in films and a larger grain size, which indicates that the crystallinity of films can be improved by appropriate Sn-doping. As the molar ratio of Sn and CdTe increases, the preferential orientation of （111） in films becomes weaker, the grain size becomes smaller, and the crystal boundary becomes indistinct, which indicates that the crystallization growth of films is incomplete. However, as the Sn content increases, optical absorption becomes stronger in the visible region. In summary, a strongly preferential orientation of （111） in films and a larger grain size can be obtained by appropriate Sn-doping （molar ratio of Sn ： CdTe = 0.06 ： 1）, while the film retains a relatively high optical absorption in the visible region. However, Sn-doping has no obvious influence on the energy gap of CdTe films.     

Effects of Sn-doping on morphology and optical properties of CdTe polycrystalline films

Sn-doped CdTe polycrystalline films were successfully deposited on ITO glass substrates by close space sublimation. The effects of Sn-doping on the microstructure, surface morphology, and optical properties of polycrystalline films were studied using X-ray diffraction, scanning electron microscopy, and ultraviolet-visible spectrophotometry, respectively. The results show that the lower molar ratio of Sn and CdTe conduces to a strongly preferential orientation of (111) in films and a larger grain size, which indicates that the crystallinity of films can be improved by appropriate Sn-doping. As the molar ratio of Sn and CdTe increases, the preferential orientation of (111) in films becomes weaker, the grain size becomes smaller, and the crystal boundary becomes indistinct, which indicates that the crystallization growth of films is incomplete. However, as the Sn content increases, optical absorption becomes stronger in the visible region. In summary, a strongly preferential orientation of (111) in films and a larger grain size can be obtained by appropriate Sn-doping (molar ratio of Sn : CdTe = 0.06 : 1), while the film retains a relatively high optical absorption in the visible region. However, Sn-doping has no obvious influence on the energy gap of CdTe films.