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Fabrication and characterization of He-charged ODS-FeCrNi films deposited by a radio-frequency plasma magnetron sputtering technique
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作者 宋亮 王先平 +6 位作者 王乐 张营 刘旺 蒋卫斌 张涛 方前锋 刘长松 《Plasma Science and Technology》 SCIE EI CAS CSCD 2017年第4期68-75,共8页
He-charged oxide dispersion strengthened (ODS) FeCrNi fills were prepared by a radiofrequency (RF) plasma magnetron sputtering method in a He and Ar mixed atmosphere at 150 °C.As a comparison,He-charged FeCrN... He-charged oxide dispersion strengthened (ODS) FeCrNi fills were prepared by a radiofrequency (RF) plasma magnetron sputtering method in a He and Ar mixed atmosphere at 150 °C.As a comparison,He-charged FeCrNi films were also fabricated at the same conditions through direct current (DC) plasma magnetron sputtering.The doping of He atoms and Y2O3 in the FeCrNi fills was realized by the high backscattered rate of He ions and Y2O3/FeCrNi composite target sputtering method,respectively.Inductive coupled plasma (ICP) and x-ray photoelectron spectroscopy (XPS) analysis confirmed the existence of Y2O3 in FeCrNi fills,and Y2O3 content hardly changed with sputtering He/Ar ratio.Cross-sectional scanning electron microscopy (SEM) shows that the FeCrNi films were composed of dense colunnarnanocrystallines and the thickness of the films was obviously dependent on He/Ar ratio.Nanoindentation measurements revealed that the FeCrNi films fabricated through DC/RF plasma magnetron sputtering methods exhibited similar hardness values at each He/Ar ratio,while the dispersion of Y2O3 apparently increased the hardness of the fills.Elastic recoil detection (ERD) showed that DC/RF magnetron sputtered FeCrNi films contained similar He amounts (~17 at.%).Compared with the minimal change of He level with depth in DC-sputtered films,the He amount decreases gradually in depth in the RF-sputtered fills.The Y2O3-doped FeCrNi films were shown to exhibit much smaller amounts of He owing to the lower backscattering possibility of Y2O3 and the inhibition effect of nano-sized Y2O3 particles on the He element. 展开更多
关键词 radio-frequency plasma magnetron sputtering He-charged FeCrNi-based film nanoindentation hardness elastic recoil detection He implantation
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固体光声效应研究 被引量:3
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作者 王阳恩 尚志远 +1 位作者 董彦武 王公正 《陕西师大学报(自然科学版)》 CSCD 北大核心 1998年第4期117-118,共2页
材料在低强度激光照射下产生光声效应的主要机理是热弹膨胀[1].激光强度较高时,照射到固体材料表面,会产生蒸发、光击穿,从而产生等离子体.作者在文[2]的基础上,从理论上研究了被蒸发的物质以一定的上升速度离开固体材料表... 材料在低强度激光照射下产生光声效应的主要机理是热弹膨胀[1].激光强度较高时,照射到固体材料表面,会产生蒸发、光击穿,从而产生等离子体.作者在文[2]的基础上,从理论上研究了被蒸发的物质以一定的上升速度离开固体材料表面时所产生的反冲压力作用,以及在这... 展开更多
关键词 固体 光声效应 激光辐射
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脉冲激光烧蚀材料等离子体反冲压力物理模型研究与应用 被引量:4
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作者 蔡颂 陈根余 +2 位作者 周聪 周枫林 李光 《物理学报》 SCIE EI CAS CSCD 北大核心 2017年第13期99-111,共13页
分析了脉冲激光烧蚀材料等离子体等温膨胀阶段的物理特性,建立了脉冲激光烧蚀材料等离子体压力三维方程与动力学模型.应用所建模型,数值分析了单脉冲激光烧蚀青铜金刚石砂轮等离子体相关特性,得到等离子体的反冲压力最大值870 Pa出现在... 分析了脉冲激光烧蚀材料等离子体等温膨胀阶段的物理特性,建立了脉冲激光烧蚀材料等离子体压力三维方程与动力学模型.应用所建模型,数值分析了单脉冲激光烧蚀青铜金刚石砂轮等离子体相关特性,得到等离子体的反冲压力最大值870 Pa出现在约25 ns后,距离砂轮表面距离约0.05 mm处.相关条件下开展脉冲激光烧蚀青铜金刚石砂轮试验,采用高速相机观测烧蚀砂轮过程中的飞溅现象;采用光栅光谱仪测量等离子体空间发射光谱,计算了等离子体电子温度、电子密度以及反冲压力.实验表明脉冲激光烧蚀青铜金刚石砂轮等离子体反冲压力可以不计,同时也验证了气体方程与动力学模型的正确性和可行性,对脉冲光纤激光烧蚀工艺优化具有启示意义. 展开更多
关键词 激光烧蚀 等离子体 青铜金刚石砂轮 反冲压力
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激光辐照固体靶产生等离子体反冲研究
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作者 周磊 李晓亚 +2 位作者 祝文军 王加祥 唐昌建 《物理学报》 SCIE EI CAS CSCD 北大核心 2016年第8期274-280,共7页
提出一种通过诊断等离子体反冲动量来计算激光加载产生冲击压强的方法.当强激光辐照固体靶表面时,所产生的高速喷射的等离子体对靶具有反冲作用,通过诊断等离子体反冲动量的变化可以计算激光辐照固体靶产生的冲击压强变化.本文利用辐射... 提出一种通过诊断等离子体反冲动量来计算激光加载产生冲击压强的方法.当强激光辐照固体靶表面时,所产生的高速喷射的等离子体对靶具有反冲作用,通过诊断等离子体反冲动量的变化可以计算激光辐照固体靶产生的冲击压强变化.本文利用辐射流体力学软件研究了这种诊断方法,模拟采用的激光功率密度为5×10^(12)—5×10^(13)W/cm^2,激光脉宽选取纳秒量级.模拟结果表明该方法是有效且可行的. 展开更多
关键词 等离子体反冲 冲击压强 激光加载 激光干涉
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Characteristics of Cu implantation into Si by PBII using UBMS cathode
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作者 于伟东 夏立芳 孙跃 《中国有色金属学会会刊:英文版》 CSCD 2001年第2期173-177,共5页
The implantation of Cu into Si substrate was carried out by plasma based ion implantation (PBII) using unbalanced magnetron sputtering (UBMS) cathode as the metal plasma source. The different pulse bias ( U p) and the... The implantation of Cu into Si substrate was carried out by plasma based ion implantation (PBII) using unbalanced magnetron sputtering (UBMS) cathode as the metal plasma source. The different pulse bias ( U p) and the distance between the cathode and the samples ( d s-t ) were chosen to research the characteristics of this method. The results show that the implantation of metal ions can be realized by the metal plasma source of UBMS cathode. The physical process such as the metal ion pure implantation, the gas ion implantation, the recoil implantation of the metal atoms, the deposition of the metal particles and the re sputtering of the metal film depend on the energy, dose and deposition rate of the ions (Cu +, Ar +). The metal plasma based ion implantation of Cu into Si substrate is favored by selecting higher U p (60 kV) and larger d s-t (200 mm). [ 展开更多
关键词 unbalanced magnetron sputtering plasma based ion implantation recoil implantation
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