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直流磁控溅射沉积含He钛膜的研究   总被引:1,自引:0,他引:1  
研究了用He/Ar混合溅射气体的直流磁控溅射制备钛膜中,He的掺入现象.分析结果表明,大量的He原子(He/Ti原子比高达56%)被均匀地引入到Ti膜中,其He含量可由混合溅射气体的He分量精确控制.通过调节溅射参数,可实现样品中He的低损伤引入.研究还发现,溅射沉积的含氦Ti膜具有较高的He成泡剂量和高的固He能力,这可能是溅射沉积形成了纳米晶Ti膜所致.纳米晶Ti膜较粗晶材料具有很高浓度的He捕陷中心,使He泡密度增大而泡尺寸减小.随He引入量的增加,Ti膜的晶粒尺寸减小,He引起的晶体点阵参数和X射线衍射峰宽度增大,晶体的无序程度增加.Helium trapping in the Ti films deposited by DC magnetron sputtering with a He/Ar mixture was studied. He atoms with a surprisingly high concentration (He/Ti atomic ratio is as high as 56%)incorporate evenly in deposited film. The trapped amount of He can be controlled by the helium partial amount. The introduction of the helium with no extra damage(or very low damage) can be realized by choosing suitable deposition conditions. It was also found that because of the formation of nanophase Ti film a relative high He flux for bubble formation is needed and the amount of the retain He in sputtering Ti films is much higher than that in the coarse grain Ti films. The nanophase Ti film can accommodate larger concentration of trapped sites to He, which results in a high density and small size of the He bubbles. With the increasing He irradiation flux, the grain size of Ti film decreases and the lattice spacing and width of the X ray diffraction peak increase due to the He introduction, and the film tends to amorphous phase.  相似文献   
2.
AgGaSe_2晶体差频产生可调谐太赫兹波的理论研究   总被引:1,自引:0,他引:1       下载免费PDF全文
基于单轴晶体中三波互作用的共线相位匹配技术,采用CO2激光器泵浦非线性晶体AgGaSe2,数值计算出在oee类和oeo类相位匹配条件下,差频产生太赫兹波的相位匹配角、走离角、允许角和有效非线性系数。计算结果表明:两类相位匹配太赫兹波可调谐的范围都非常宽,而且走离角都在1°以下,允许角足够大。在绝大部分太赫兹波区域,oee类匹配有效非线性系数远大于oeo类匹配,实验中适合采用oee类相位匹配方式。  相似文献   
3.
通过在石墨烯超表面设计周期性切条,实现了基于石墨烯互补超表面的可调谐太赫兹吸波体.通过改变外加电压来改变石墨烯的费米能级,吸波体实现频率可调谐特性.研究了石墨烯费米能级、结构尺寸对超材料吸波体吸收特性的影响,并利用多重反射理论研究了其物理机理并且证明了模拟方法的可行性.研究结果表明:当石墨烯费米能级取0.6 eV,基底厚度13μm,石墨烯上切条长宽分别为2.9μm,0.1μm时,吸波体在1.865 THz可以实现99.9%的完美吸收;石墨烯费米能级从0.4 eV增大到0.9 eV,吸波体共振频率从1.596 THz蓝移到2.168 THz,且伴随共振吸收率的改变,吸收率在0.6 eV时达到最大;通过改变费米能级实现的最大吸收率调制度达84.55%.  相似文献   
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A face-to-face system of double-layer three-dimensional arrays of H-shaped plasmonic crystals is proposed, and its transmission and filtering properties are investigated in the terahertz regime. Simulation results show that our design has excellent filtering properties. It has an ultra-wide bandgap and passband with steep band-edges, and the transmittance of the passband and the forbidden band are very close to I and 0, respectively. As the distance between the two face-to-face plates increases, the resonance frequency exhibits a gradual blueshift from 0.88 THz to 1.30 THz. Therefore, we can dynamically control the bandwidths of bandgap and passband by adding a piezoelectric ceramic plate between the two crystal plates. Furthermore, the dispersion relations of modes and electric field distributions are presented to analyze the generation mechanisms of bandgaps and to explain the location of bandgaps and the frequency shift phenomenon. Due to the fact that our design can provide many resonant modes, the bandwidth of the bandgaps can be greatly broadened. This paper can serve as a valuable reference for the design of terahertz functional devices and three-dimensional terahertz metamaterials.  相似文献   
5.
袁偲  徐世林  姚建铨  赵晓蕾  曹小龙  吴亮 《中国物理 B》2014,23(1):18102-018102
A face-to-face system of double-layer three-dimensional arrays of H-shaped plasmonic crystals is proposed, and its transmission and filtering properties are investigated in the terahertz regime. Simulation results show that our design has excellent filtering properties. It has an ultra-wide bandgap and passband with steep band-edges, and the transmittance of the passband and the forbidden band are very close to 1 and 0, respectively. As the distance between the two face-to-face plates increases, the resonance frequency exhibits a gradual blueshift from 0.88 THz to 1.30 THz. Therefore, we can dynamically control the bandwidths of bandgap and passband by adding a piezoelectric ceramic plate between the two crystal plates. Furthermore, the dispersion relations of modes and electric field distributions are presented to analyze the generation mechanisms of bandgaps and to explain the location of bandgaps and the frequency shift phenomenon. Due to the fact that our design can provide many resonant modes, the bandwidth of the bandgaps can be greatly broadened. This paper can serve as a valuable reference for the design of terahertz functional devices and three-dimensional terahertz metamaterials.  相似文献   
6.
The thin film metal hydride has become an emerging field of research in metal hydride batteries for its good mechanical and hydrogenation properties. ZrV2 thin films have been prepared using a dc magnetron sputtering method, and the phase structure is investigated. Only amorphous or crystalline Zr and V mixture phases are achieved when substrates are heated during either to 400℃ or to 550℃. The annealing causes segregation of Zr and V in the film induced by strain-driven diffusion and interdiffusion between substrate Mo and film elements at high temperature, which results in the formation of mixture phases ofC14, C15, Zr and V, but the content of C15 phase is not higher compared with that in the bulk material.  相似文献   
7.
为研究远场爆炸荷载作用下单向砌体填充墙的动力行为及其失效破坏机理,首先,基于研发的压缩空气驱动大截面(3 m×3 m)激波管开展了两面不同厚度单向实心砌体填充墙的面外加载试验,获得了作用在墙体表面的反射超压荷载时程、墙体面外挠度时程及墙体的变形失效模式。其次,建立了激波管精细化有限元模型,提出了砌体墙简化微观有限元建模方法,以及扩展砖块的Riedel-Hiermaier-Thoma材料模型和接缝的内聚力接触模型参数取值计算方法,对激波管中的压力传播以及试验墙体面外动态响应和损伤破坏开展了数值模拟。最后,基于爆炸荷载作用下单向砌体填充墙面外抗力方程和等效单自由度模型对试验墙体中心点面外挠度时程进行预测。结果表明:减小墙体高厚比可以增大框架拱推力,从而显著提升墙体的抗爆性能,厚105 mm的墙体在经历1次激波管试验后发生倒塌,而厚235 mm的墙体在经历6次激波管试验后仅有轻微损伤;墙体表面反射超压荷载时程的试验和数值模拟结果均为均布脉冲型荷载,且两者吻合很好,验证了激波管设计和激波管精细化有限元模型的合理性;数值模拟和理论预测的墙体动力行为与试验结果吻合较好,可为砌体填充墙抗爆评估与分析...  相似文献   
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