排序方式: 共有12条查询结果,搜索用时 31 毫秒
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采用中红外CO2激光差频产生太赫兹波是提高转换效率和输出功率的一种有效方法。根据差频过程中的三波互作用对AgGaS2晶体进行了理论分析,数值模拟了oeo类和oee类两种匹配条件下差频产生太赫兹波的角度调谐曲线,并计算了光波在晶体中的走离角和允许参量。另外,还考虑了晶体的有效非线性系数和理论功率转换效率。研究结果表明,AgGaS2晶体适用于中红外CO2激光差频产生可广泛调谐的太赫兹波。 相似文献
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基于腔相位匹配的方法,研究了GaAs微片状晶体构成的光学微腔光参量振荡产生太赫兹波的条件与参数设计.计算了腔相位匹配下GaAs晶体的最优化腔长,通过调节GaAs晶体的温度研究了太赫兹波的输出情况,模拟了不同波长下最低的能量阈值.结果表明,在完全相位匹配很难实现的情况下,采用腔相位匹配能很容易地实现大范围的太赫兹波调谐输出.结果为小型化光学太赫兹源的实验与理论研究提供了参考. 相似文献
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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
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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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石墨烯特殊的零带隙能带结构和载流子弛豫特性,在研究太赫兹辐射源相干放大领域引起广泛关注。考虑带内和带间跃迁对电导率的贡献,研究了光抽运单层和多层石墨烯中非平衡二维电子-空穴系统的动态电导率特性。结果表明,在足够强的光抽运下,石墨烯中的粒子数反转能够使得动态电导率的实部在太赫兹频段内出现负值,这使基于石墨烯的太赫兹放大或受激辐射源成为可能。同时,通过研究动量弛豫时间、温度、层数、光强对石墨烯的负动态电导率的影响表明,石墨烯多层结构的动态电导率最小值的绝对值更大,作为太赫兹激光器的激活介质更具优势。 相似文献
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Tunable ultra-wideband terahertz filter based on three-dimensional arrays of H-shaped plasmonic crystalsTunable ultra-wideband terahertz filter based on three-dimensional arrays of H-shaped plasmonic crystalsTunable ultra-wideband terahertz filter based on three-dimensional arrays of H-shaped plasmonic crystals
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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
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Tunable ultra-wideband terahertz filter based on three-dimensional arrays of H-shaped plasmonic crystals
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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 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
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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