退火温度和溅射时间对磁控溅射法制备Mg2Si薄膜的影响

采用磁控溅射法和原位退火工艺在钠钙玻璃衬底上制备 Mg2Si 薄膜。首先在钠钙玻璃衬底上交替溅射沉积两层Si、Mg 薄膜,冷却至室温后原位退火4 h,制备出一系列 Mg2Si 薄膜样品。通过 X 射线衍射仪(XRD) 、 扫描电子显微镜(SEM)对所得薄膜样品的晶体结构和表面形貌进行表征, 讨论了退火温度和溅射Si/Mg/Si/Mg 时间对制备 Mg2Si 薄膜的影响。结果表明,采用磁控溅射法在钠钙玻璃衬底上交替溅射两层Si、Mg 薄膜, 通过原位退火方式成功制备出单一相的 Mg2Si 薄膜,溅射Si/Mg/Si/Mg 的时间为12.5/9/12.5/9 min,退火温度为550 ℃ 时,制备的 Mg2Si 薄膜结晶度最好,连续性和致密性最强。这对后续 Mg2Si 薄膜器件的设计与制备提供了重要的参考。 积两层Si、Mg 薄膜, 冷却至室温后原位退火4 h, 制备出一系列 Mg2Si 薄膜样品. 通过 X 射线衍射仪(XRD) 、 扫描 电子显微镜(SEM)对所得薄膜样品的晶体结构和表面形貌进行表征, 讨论了退火温度和溅射Si/Mg/Si/Mg 时间 对制备 Mg2Si 薄膜的影响. 结果表明, 采用磁控溅射法在钠钙玻璃衬底上交替溅射两层Si、Mg 薄膜, 通过原位退火 方式成功制备出单一相的 Mg2Si 薄膜, 溅射Si/Mg/Si/Mg 的时间为12.5/9/12.5/9 min, 退火温度为550 ℃ 时, 制 备的 Mg2Si 薄膜结晶度最好, 连续性和致密性最强. 这对后续 Mg2Si 薄膜器件的设计与制备提供了重要的参考.     

脉冲激光沉积法制备的ZnO薄膜的低阈值电抽运紫外随机激射

分别采用直流反应溅射法和脉冲激光沉积法在硅衬底上沉积ZnO薄膜, 用X射线衍射、扫描电镜、光致发光谱等手段对两种方法沉积的ZnO薄膜的结晶状态、 表面形貌和光致发光等进行了表征. 进一步对比研究了以上述两种方法制备的ZnO薄膜作为发光层的金属-绝缘体-半导体结构器件的电抽运紫外随机激射. 结果表明, 与以溅射法制备的ZnO薄膜作为发光层的器件相比, 以脉冲激光沉积法制备的ZnO薄膜为发光层的器件具有更低的紫外光随机激射阈值电流和更高的输出光功率. 这是由于脉冲激光沉积法制备的ZnO薄膜中的缺陷更少, 从而显著地减少了紫外光在光散射过程中的光损耗. 关键词： 随机激射 ZnO薄膜 脉冲激光沉积 溅射     

FTIR法研究BCN薄膜的内应力

采用射频磁控溅射技术,用六角氮化硼和石墨为溅射靶,以氩气(Ar)和氮气(N₂)为工作气体,在Si(100)衬底上制备出硼碳氮(BCN)薄膜。利用傅里叶变换红外光谱(FTIR)考察了不同沉积参数(溅射功率为80～130 W、衬底温度为300～500 ℃、沉积时间为1～4 h)条件下制备的薄膜样品。实验结果表明,所制备薄膜均实现了原子级化合。并且沉积参数对BCN薄膜的生长和内应力有很大影响,适当改变沉积参数能有效释放BCN薄膜的内应力。在固定其他条件只改变一个沉积参数的情况下,得到制备具有较小内应力的硼碳氮薄膜的最佳沉积条件：溅射功率为80 W、衬底温度为400 ℃、沉积时间为2 h。     

NbN薄膜的制备与性能研究

采用磁控溅射和直流偏压二极溅射两种方法制备了NbN薄膜。用XRD和TEM测量比较了两种不同溅射方法获得的NbN薄膜的特点,并测量了NbN薄膜的超导转变温度T_c。采用两种溅射方法都得到了致密、均匀、单一δ相的多晶NbN薄膜,薄膜生长的择优取向受温度和氮气流量的影响很大,薄膜的超导转变温度受溅射室本底真空影响较大。     

用磁控溅射法制备Cu薄膜的研究

采用磁控溅射法在玻璃衬底上制备了Cu薄膜 ,应用台阶仪测量Cu膜的厚度 ,研究了薄膜的沉积速率与溅射功率的关系 ;用X射线衍射 (XRD)和扫描电镜Cu对薄膜进行了表征 ,研究了溅射功率对所制备薄膜的影响。制备出致密性和均匀性较好的Cu薄膜。     

聚电解质/硫化镉薄膜的层-层组装及其光谱分析

以六偏磷酸钠为稳定剂,采用硝酸镉和硫化钠合成了硫化镉纳米颗粒,利用层-层组装技术制备了聚电解质与硫化镉胶体的复合薄膜.吸收光谱显示,硫化镉胶体的吸收带边相对其体相有明显蓝移,并可观察到激子吸收峰,显示出量子尺寸效应.复合薄膜的荧光光谱上出现2个发光带,随着薄膜的组装层数的增加,复合薄膜的带带跃迁发光和表面态发光都相应减弱.     

溅射功率对Mo薄膜微结构和性能的影响

 实验采用直流磁控溅射沉积技术在不同溅射功率下制备Mo膜,研究了不同溅射功率下Mo膜的沉积速率、表面形貌及晶型结构,并对其晶粒尺寸和应力进行了研究。利用原子力显微镜观察样品的表面形貌发现随着溅射功率的增加,薄膜表面粗糙度逐渐增大。X射线衍射分析表明薄膜呈立方多晶结构,晶粒尺寸为14.1～17.9 nm;应力先随溅射功率的增大而增大,在40 W时达到最大值(2.383 GPa),后随溅射功率的增大有所减小。     

Ge-Sb-Se硫系薄膜制备及光学特性研究

介绍了几种常见的硫系薄膜制备方法, 根据现有实验条件采用热蒸发法和磁控溅射法制备出Ge-Sb-Se三元体系硫系薄膜, 通过台阶仪测试薄膜的厚度和表面粗糙度, 计算出两种制备方法的成膜速率, 并通过X射线光电子能谱测试了两种制备方法所得薄膜与块体靶材组分的差别. 利用Z扫描技术和分光光度计测试了热蒸发法制备所得薄膜的三阶非线性性能和透过光谱, 计算出非线性折射率、非线性吸收系数和薄膜厚度等参数. 结果表明热蒸发法制备Ge-Sb-Se薄膜具有良好的物理结构和光学特性, 在集成光学器件方面很高的应用潜力.     

脉冲溅射功率对含硅量子点SiC_x薄膜的结构和光学特性的影响

采用射频和脉冲磁控共溅射法并结合快速光热退火法制备了含硅量子点的SiC_x薄膜.采用掠入射X射线衍射、喇曼光谱、紫外-可见-近红外分光光度计和透射电子显微镜对薄膜进行表征.研究了脉冲溅射功率对薄膜中硅量子点数量、尺寸、晶化率和薄膜光学带隙的影响.结果表明:当溅射功率从70 W增至100 W时,硅量子点数量增多,尺寸增至5.33nm,晶化率增至68.67%,而光学带隙则减至1.62eV;随着溅射功率进一步增至110 W时,硅量子点数量减少,尺寸减至5.12nm,晶化率降至55.13%,而光学带隙却增至2.23eV.在本实验条件下,最佳溅射功率为100 W.     

射频磁控溅射法制备的Eu掺杂ZnO薄膜的结构及其发光性质

用射频磁控溅射法在石英衬底上制备了ZnO:Eu3+薄膜,通过X射线衍射仪、扫描电子显微镜和荧光光谱仪测试了薄膜结构、形貌以及发光性能,重点考察了溅射功率和退火工艺对其组织结构和发光性能的影响.结果表明:样品均呈现ZnO的六角纤锌矿结构,增大溅射功率有利于形成ZnO的c轴择优取向;增大溅射功率以及高温退火会使晶粒尺寸增大...     

退火对ZnO薄膜光学特性的影响

用射频磁控溅射法在蓝宝石衬底上制备出ZnO薄膜,通过X射线衍射(XRD)、扫描电镜(SEM)和光致发光(PL)谱等研究了退火温度对ZnO薄膜结构和光学性质的影响。测量结果显示,所制备的ZnO薄膜为六角纤锌矿结构,具有沿c轴的择优取向;随着退火温度的升高,(002)XRD峰强度和平均晶粒尺寸增大,(002)XRD峰半高宽(FWHM)减小,光致发光紫外峰强度增强。结果证明,用射频磁控溅射法通过适当控制退火温度可得到高质量ZnO薄膜。     

不同衬底和CdCl2退火对磁控溅射CdS薄膜性能的影响

在科宁7059玻璃, FTO, ITO, AZO四种衬底上磁控溅射CdS薄膜, 并在CdCl₂+干燥空气380 ℃退火, 分别研究了不同衬底和退火工艺对CdS薄膜形貌、结构和光学性能的影响. 扫描电子显微镜形貌表明: 不同衬底原位溅射CdS薄膜的形貌不同, 退火后相应CdS薄膜的晶粒度和表面粗糙度明显增大. XRD衍射图谱表明: 不同衬底原位溅射和退火CdS薄膜均为六角相和立方相的混相结构, 退火前后科宁7059玻璃, FTO, AZO衬底上CdS薄膜有 H(002)/C(111) 最强衍射峰, ITO衬底原位溅射CdS薄膜没有明显的最强衍射峰, 退火后出现 H(002)/(111) 最强衍射峰. 紫外-可见分光光度计分析表明: AZO, FTO, ITO, 科宁7059玻璃衬底CdS薄膜的可见光平均透过率依次减小, 退火后相应衬底CdS薄膜的可见光平均透过率增大, 光学吸收系数降低; 退火显著增大了不同衬底CdS薄膜的光学带隙. 分析得出: 上述结果是由于不同衬底类型和退火工艺对CdS多晶薄膜的形貌、结构和带尾态掺杂浓度改变的结果. 关键词： CdS薄膜 磁控溅射 退火再结晶 带尾态     

退火温度对低温生长MgxZn1－xO薄膜光学性质的影响

用射频磁控溅射法在80℃衬底温度下制备出Mg_xZn_1-xO(x=0.16)薄膜，用X射线衍射(XRD)、光致发光(PL)和透射谱研究了退火温度对Mg_xZn_1-xO薄膜结构和光学性质的影响.测量结果显示，Mg_xZn_1-xO薄膜为单相六角纤锌矿结构，并且具有沿c轴的择优取向；随着退火温度的升高，(002)XRD峰强度、平均晶粒尺寸和紫外PL峰强度增大，(002)XRD峰半高宽(F 关键词： xZn_1-xO薄膜')" href="#">Mg_xZn_1-xO薄膜 射频磁控溅射 退火     

Photoluminescence studies on nanostructured cadmium sulfide thin films prepared by chemical bath deposition method and annealed at different temperatures

Nanostructured cadmium sulfide (CdS) thin films have been prepared by chemical bath deposition (CBD) method and after post deposition annealing of the thin films at different temperatures, photoluminescence (PL) property has been studied. The effects of various photoexcitation wavelengths on the PL behaviour of different annealed films of CdS were studied by recording the PL spectra. The intensity of PL, the profile of the PL spectra and the effects of photoexcitation wavelength depend drastically on the temperature of the post deposition annealing of the thin films. The XRD patterns of the films show the presence of both the hexagonal and cubic phases (mixed phases). The emission peak arises from the surface defects of the CdS nanocrystalline thin films. Significant modification in the surface morphology of the CdS films upon annealing has been observed from the FESEM images. The morphology of the thin films is expected to influence the PL behaviour of the CdS thin films. The quantum size effect and size dependant PL have been observed.     

The comparison between CdS thin films grown on Si(111) substrate and quartz substrate by femtosecond pulsed laser deposition

Two kinds of cadmium sulfate (CdS) thin films have been grown at 600 °C onto Si(111) and quartz substrates using femtosecond pulsed laser deposition (PLD). The influence of substrates on the structural and optical properties of the CdS thin films grown by femtosecond pulsed laser deposition have been studied. The CdS thin films were characterized by X-ray diffraction (XRD), atomic force microscopy (AFM), scanning electron microscopy (SEM), photoluminescence (PL) and Raman spectroscopy. Although CdS thin films deposited both on Si(111) and quartz substrates were polycrystalline and hexagonal as shown by the XRD , SEM and AFM results, the crystalline quality and optical properties were found to be different. The size of the grains for the CdS thin film grown on Si(111) substrate were observed to be larger than that of the CdS thin film grown on quartz substrate, and there is more microcrystalline perpendicularity of c-axis for the film deposited on the quartz substrate than that for the films deposited on the Si substrate. In addition, in the PL spectra, the excitonic peak is more intense and resolved for CdS film deposited on quartz than that for the CdS film deposited on Si(111) substrate. The LO and TO Raman peaks in the CdS films grown on Si(111) substrate and quartz substrate are different, which is due to higher stress and bigger grain size in the CdS film grown on Si(111) substrate, than that of the CdS film grown on the amorphous quartz substrate. All this suggests that the substrates have a significant effect on the structural and optical properties of thin CdS films. PACS 81.15.Fg; 81.05.Ea; 78.20.-e; 78.67.-n; 42.62.-b     

Deposition of quasi-crystal Al-doped ZnO thin films for photovoltaic device applications

Quasi-crystal aluminum-doped zinc oxide (AZO) films were prepared by in situ radio frequency (RF) magnetron sputtering (sputtering without annealing) on glass substrates. The influence of deposition parameters on the optoelectronic and structural properties of the in situ deposited quasi-crystal AZO films was investigated in order to compare resulting samples. X-ray diffraction (XRD) patterns show that the quasi-crystal AZO thin films have excellent crystallization improved with increase of the RF power and substrate temperature, with an extremely preferential c-axis orientation exhibit sharp and narrow XRD pattern similar to that of single-crystal. Field emission scanning electron microscopy (FESEM) images show that quasi-crystal AZO thin films have uniform grains and the grain size increase with the increase of RF power and substrate temperature. Craters of irregular size with the columnar structure are observed in the quasi-crystal AZO thin films at a lower substrate temperature while many spherical shaped grains appeared at a higher substrate temperature. The average optical transmittance of all the quasi-crystal AZO films was over 85% in the 400-800 nm wavelength range. The resistivity of 4.176 × 10⁻⁴ Ω cm with the grain size of 76.4891 nm was obtained in the quasi-crystal AZO thin film deposited at 300 °C, under sputtering power of 140 W.     

射频磁控溅射法制备SnS薄膜及其结构和光学特性

利用射频磁控溅射法在玻璃衬底上沉积SnS薄膜并对其进行快速退火处理,利用X射线衍射(XRD)、拉曼光谱(Raman)、X射线能量色散谱(EDS)、原子力显微镜(AFM)和紫外-可见-近红外(UV-Vis-NIR)分光光度计研究了不同溅射功率(60~120 W)条件下制备的SnS薄膜的晶体结构、物相组成、化学组分、表面形貌以及有关光学特性。结果表明:经快速退火的薄膜均已结晶,提高溅射功率有利于改善薄膜的结晶质量、生长择优取向程度和化学配比,薄膜的平均颗粒尺寸呈增大趋势;溅射功率为100 W的薄膜样品的结晶质量和择优取向度高,薄膜应变最小,且为纯相SnS薄膜,Sn/S组分的量比为1∶1.09,吸收系数达10~5cm~(-1)量级,直接禁带宽度为1.54 eV。     

RF magnetron sputtering induced the perpendicular magnetic anisotropy modification in Pt/Co based multilayers

We demonstrate that radio frequency(RF)magnetron sputtering technique can modify the perpendicular magnetic anisotropy(PMA)of Pt/Co/normal metal(NM)thin films.Influence of ion irradiation during RF magnetron sputtering should not be neglected and it can weaken PMA of the deposited magnetic films.The magnitude of this influence can be controlled by tuning RF magnetron sputtering deposition conditions and the upper NM layer thickness.According to the stopping and range of ions in matter(SRIM)simulation results,defects such as displacement atoms and vacancies in the deposited film will increase after the RF magnetron sputtering,which can account for the weakness of PMA.The amplitude changes of the Hall resistance and the threshold current intensity of spin orbit torque(SOT)induced magnetization switching also can be modified.Our study could be useful for controlling magnetic properties of PMA films and designing new type of SOT-based spintronic devices.     

感应耦合等离子体增强射频磁控溅射沉积ZrN薄膜及其性能研究

利用感应耦合等离子体(ICP)增强射频磁控溅射技术在Si(111)片和M2钢表面制备了ZrN薄膜,研究了基片的温度和ICP功率对ZrN薄膜的结构以及性能影响.研究发现：在基片温度≤300℃沉积的ZrN薄膜择优取向为(111);基片温度达到450℃时薄膜出现ZrN(200)衍射峰,ZrN(111)晶面的织构系数明显降低.传统磁控溅射沉积薄膜为柱状结构,当ICP为200 W,基片温度为300℃时沉积薄膜中柱状晶体消失;随着基片温度的升高,N/Zr元素比例降低,并且薄膜的电阻率下降;相对于传统溅射,ICP增强射 关键词： 感应耦合等离子体 磁控溅射 ZrN 微结构     

磁控溅射沉积薄膜实验参数优化光谱诊断

采用磁控溅射仪、Omni-λ300系列光栅光谱仪、CCD数据采集系统和光纤导光系统等构成的等离子体光谱分析系统,采集了以Cu和Al为靶材、氩气为工作气体,射频磁控溅射法沉积硅基薄膜时的等离子体发射光谱。以CuⅠ324.754 nm,CuⅠ327.396 nm,CuⅠ333.784 nm,CuⅠ353.039 nm,AlⅠ394.403 nm和AlⅠ396.153 nm为分析线,研究了Cu和Al等离子体发射光谱强度随溅射时间、溅射功率、靶基距和气体压强等实验参数的变化。并与射频磁控溅射沉积薄膜实验参数的选择进行对比,表明发射光谱法对射频磁控溅射薄膜生长条件的优化有着很好的指导作用。