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 共查询到16条相似文献,搜索用时 49 毫秒
1.
李红凯  林国强  董闯 《物理学报》2008,57(10):6636-6642
用脉冲偏压电弧离子镀通过控制不同的氮流量在(100)单晶Si基片上制备了不同成分的CNx薄膜.用光学显微镜,XPS,XRD,激光Raman和Nanoindenter等方法研究了薄膜的形貌、成分、结构和性能.结果表明,薄膜表面平整致密、氮含量随着氮流量的降低而降低、结构为非晶且为类金刚石薄膜;随着氮含量从18.9%降低到5.3%(摩尔百分比,全文同),薄膜的硬度和弹性模量单调增加而且增幅较大,其中硬度从15.0 GPa成倍增加到30.0 GPa;通过氮流量的调整能够敏感地改变薄膜中的sp3键的含量,是CNx薄膜的硬度和弹性模量获得大幅度调整的本质原因. 关键词x薄膜')" href="#">CNx薄膜 脉冲偏压 电弧离子镀 硬度  相似文献   

2.
张敏  林国强  董闯  闻立时 《物理学报》2007,56(12):7300-7308
用脉冲偏压电弧离子镀技术在玻璃基片上制备均匀透明的TiO2薄膜.利用X射线衍射仪、原子力显微镜、扫描电子显微镜、紫外-可见透射光谱仪和纳米压痕仪等手段,对不同脉冲负偏压下合成薄膜的相结构、微观结构、表面形貌、力学和光学性能进行表征.结果表明,沉积态薄膜为非晶态.脉冲负偏压对薄膜性能有明显的影响.随偏压的增加,薄膜厚度、硬度和弹性模量均先增大后减小,前者峰值出现在100—200 V负偏压范围,后两者则在250—350V范围.300 V负偏压时薄膜硬度最高,薄膜达到原子级表面光滑度,均方 关键词: 2薄膜')" href="#">TiO2薄膜 脉冲偏压电弧离子镀 硬度 折射率  相似文献   

3.
刘海永  张敏  林国强  韩克昌  张林 《物理学报》2015,64(13):138104-138104
采用脉冲偏压电弧离子镀技术在单晶硅基片及石英玻璃上制备了一系列均匀透明的Cr-O薄膜. 用场发射扫描电子显微镜、X射线衍射仪、X射线光电子谱、纳米压痕仪、紫外可见光分光光度计等方法对薄膜的表面形貌、膜厚、相结构、成分、元素的化学价态、硬度和光学性能等进行表征, 主要研究了偏压幅值对薄膜结构和性能的影响. 结果表明, 施加偏压可使薄膜的沉积质量明显提高, 其相结构由非晶态转变为晶体态, 并随着偏压幅值的增加, 由Cr2O3相向CrO相转变; 薄膜的硬度先增大后减小, 当偏压为-300 V时, 硬度达到最大值24.4 GPa; 薄膜具有良好的透光率, 最高可达72%; 当偏压为-200 V时, 薄膜的最大光学帯隙为1.88 eV.  相似文献   

4.
李红凯  林国强  董闯 《物理学报》2010,59(6):4296-4302
用脉冲偏压电弧离子镀方法在硬质合金基体上制备了一系列不同成分的C-N-V薄膜.用X射线光电子能谱、激光Raman光谱、 X射线衍射(XRD)、透射电子显微镜(TEM)和纳米压痕等方法分别研究了薄膜的成分、结构与性能.Raman光谱,XRD和TEM结果表明,所制备的薄膜为在类金刚石(DLC)非晶基体上匹配有VN晶体的碳基复合薄膜.随V和N含量的增加,薄膜硬度与弹性模量先增加后下降,在N含量为204%,V含量为218%时薄膜硬度与弹性模量具有最大值,分别为368和5697 GPa,高于相同条件下制备的 关键词: C-N-V薄膜 类金刚石薄膜 纳米复合薄膜 电弧离子镀  相似文献   

5.
磁控溅射CNx薄膜的附着力、粗糙度与衬底偏压的关系   总被引:5,自引:0,他引:5  
对磁控溅射生长在单晶Si(001)衬底上的CNx薄膜的附着力、粗糙度与衬底偏压的关系进行了研究。CNx薄膜沉积实验在纯N2的环境下进行.衬底温度(Ts)保持在350℃.衬底偏压(Vb)在0~-150V之间变化。利用原子力显微镜(AFM)和划痕试验机来测量CNx薄膜的表面粗糙度及对衬底的附着力。AFM和划痕实验的结果显示衬底偏压Vb对CNx薄膜的附着力和表面粗糙程度的影响很大,在-100V偏压下生长的CNx薄膜表面最光滑(粗糙度最小),同时对Si(001)衬底的附着力最好。最后根据实验结果确定了在单晶Si(001)衬底上生长光滑而且附着力好的CNx薄膜的最佳实验条件。  相似文献   

6.
7.
脉冲直流偏压增强的高质量立方氮化硼薄膜的合成   总被引:1,自引:0,他引:1       下载免费PDF全文
田晶泽  吕反修  夏立芳 《物理学报》2001,50(11):2258-2262
采用磁增强活性反应离子镀系统成功地合成了立方氮化硼薄膜.通过给基片施加脉冲直流偏压以代替传统的射频偏压,增强了立方氮化硼的成膜稳定性,研究了基片的直流脉冲偏压、等离子体放电电流、通入气体流量比(Ar/N2)和基片温度沉积参数对立方氮化硼薄膜形成的影响规律.结果表明:随着基片负偏压和放电电流的增大,薄膜中立方氮化硼的纯度提高,当基片负偏压为155V,放电电流为15A时,可获得几乎单相的立方氮化硼薄膜.基片温度为500℃和Ar/N2流量比为10时,最有利于立方氮化硼 关键词: 立方氮化硼 活性反应离子镀 脉冲偏压  相似文献   

8.
反应性离子镀制备多层薄膜   总被引:1,自引:0,他引:1  
  相似文献   

9.
 利用分离靶电弧离子镀工艺在高速钢基体上制备TiNbN多元硬质薄膜,利用TEMP-6型强流脉冲离子束(HIPIB)设备,采用含C/H离子、加速电压300 kV、脉冲宽度70 ns、束流密度60 A/cm2的强流脉冲离子束对所制备的薄膜进行辐照处理,研究辐照前后膜层的摩擦磨损性能的变化。实验结果表明:HIPIB辐照以后,薄膜的表面熔化,摩擦系数降低,晶粒细化,膜层的硬度由HK3444提高到HK3820,膜基结合力由59 N提高到65 N。在测试载荷300 N和600 N条件下,薄膜的摩擦磨损性能均有较大改善。  相似文献   

10.
高温退火对非晶CNx薄膜场发射特性的影响   总被引:1,自引:0,他引:1       下载免费PDF全文
采用射频磁控溅射方法在纯N2气氛中沉积了非晶CNx薄膜样品,并在真空中退火至900 ℃.对高温退火引起的CNx薄膜化学成分、键合结构及其场发射特性方面的变化进行研究.用傅里叶变换红外光谱和x射线光电子能谱分析样品的内部成分及键合结构的变化,其中sp2键及薄膜中N的含量与薄膜的场发射特性密切相关.退火实验的结果表明高温退火可以导致CNx薄膜中N含量大量损失,并在薄膜中形成大量sp2键,这些化学成分及键合结构上的变化将直接影响CNx薄膜的场发射特性.与其他温度退火样品相比,750 ℃退火的样品具有最低的阈值电场,显示出较好的场发射特性.  相似文献   

11.
In this work, the effect of modulation period (Λ) on Ti/TiN multilayer films deposited on high-speed-steel (HSS) substrates using pulse biased arc ion plating is reported. The crystallography structures and cross-sectional morphology of Ti/TiN multilayer films were characterized by X-ray diffraction analysis (XRD) and scanning electron microscopy (SEM), respectively. Their mechanical properties were determined via nanoindentation measurements, while the film/substrate adhesion via the scratch test. It was found that the highest hardness value reached 43 GPa for the modulation period of 54 nm, while the film/substrate adhesion also reached the highest value of 83 N. Furthermore, the hardness enhancement mechanism in the multilayer films is discussed.  相似文献   

12.
(Cr, Al)N films were deposited by pulsed bias arc ion plating on HSS and 316L stainless steel substrates. With pulsed substrate bias ranging from −100 V to −500 V, the effect of pulsed bias on film composition, phase structure, deposition rate and mechanical properties was investigated by EDX, XRD, SEM, nanoindentation and scratch measurements. The high-temperature (up to 900 °C) oxidation resistance of the films was also evaluated. The results show that Al contents and deposition rates decrease with increasing pulsed bias and the ratio of (Cr + Al)/N is almost constant at 0.95. The as-deposited (Cr, Al)N films crystallize in the pseudo-binary (Cr, Al)N and Al phases. The film hardness increases with increasing bias and reaches the maximum 21.5 GPa at −500 V. The films deposited at −500 V exhibit a high adhesion force, about 70 N, and more interestingly good oxidation resistance when annealed in air at 900 °C for 10 h.  相似文献   

13.
Thin films of titanium nitride (TiN) were deposited on stainless steel substrates by a modified deposition technique, double-layered shielded arc ion plating with vicarious circular holes (DL-SAIP). The results show that the TiN film with the distance of 10 mm between the double-layered shield plates had the least droplets. The deposition rate of the films prepared with the new technique was more homogeneous than that of all the other shielded arc ion plating. The film/substrate adhesion and microhardness values of the TiN films were higher than 40 N and 18 GPa, respectively. Thus such TiN thin films can be expected in applications.  相似文献   

14.
张国平  王兴权  吕国华  周澜  黄骏  陈维  杨思泽 《中国物理 B》2013,22(3):35204-035204
ZrN/TiZrN multilayer are deposited by cathodic vacuum arc method with different substrate bias (from 0 to -800 V), using Ti and Zr plasma flows in residual N2 atmosphere, combined with ion bombardment of sample surfaces. The effect of pulsed bias on structure and properties of films is investigated. Microstructure of the coating is analyzed by X-ray diffraction (XRD), and scanning electron microscopy (SEM). Meanwhile, the nanohardness, Young's modulus, and scratch tests are performed. The experimental results show that the films exhibit a nanoscale multilayer structure consisting of TiZrN and ZrN phases. Solid solutions are formed for component TiZrN films. The dominant preferred orientation of TiZrN films is (111) and (220). At pulsed bias of -200 V, the nanohardness and the adhesion strength of ZrN/TiZrN multilayer reach a maximum of 38 GPa, and 78 N, respectively. The ZrN/TiZrN multilayer demonstrates an enhanced nanohardness compared with binary TiN and ZrN films deposited under equivalent conditions.  相似文献   

15.
ZrN/TiZrN multilayers are deposited by using the cathodic vacuum arc method with different substrate bias(from 0 to 800 V),using Ti and Zr plasma flows in residual N 2 atmosphere,combined with ion bombardment of sample surfaces.The effect of pulsed bias on the structure and properties of films is investigated.Microstructure of the coating is analyzed by X-ray diffraction(XRD),and scanning electron microscopy(SEM).In addition,nanohardness,Young’s modulus,and scratch tests are performed.The experimental results show that the films exhibit a nanoscale multilayer structure consisting of TiZrN and ZrN phases.Solid solutions are formed for component TiZrN films.The dominant preferred orientation of TiZrN films is(111) and(220).At a pulsed bias of 200 V,the nanohardness and the adhesion strength of the ZrN/TiZrN multilayer reach a maximum of 38 GPa,and 78 N,respectively.The ZrN/TiZrN multilayer demonstrates an enhanced nanohardness compared with binary TiN and ZrN films deposited under equivalent conditions.  相似文献   

16.
反应离子镀光学薄膜的微观结构分析   总被引:1,自引:1,他引:1  
王建成  韩丽瑛 《光学学报》1993,13(10):56-959
用反应离子镀方法制备了TiO2单层膜及TiO2/SiO2多层膜,用透射电子显微镜分别观察了由反应离子镀方法及传统蒸镀法二种不同工艺制得的TiO2单层膜及TiO2/SiO2多层膜的断面结构,并对TiO2单层膜进行了喇曼分析和卢瑟福背散射分析。  相似文献   

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