共查询到18条相似文献,搜索用时 156 毫秒
1.
与单纯的磁光晶体相比,由磁光介质与电介质周期性或准周期性排列构成的一维磁光光子晶 体能够显著增强磁光效应,可以用于实现小尺度的磁光隔离器,从而大大减小器件的尺寸. 给出更为一般的可用于求解斜入射情况下偏振光在各向异性介质中传播时的传输矩阵方法, 并用这种方法在波长为1053μm处,针对两种“三明治”型的反射磁光多层膜隔离器的 结构,具体讨论了器件应用时入射角度及工艺制作时膜层制备厚度对它们工作稳定性的影响 .发现中心磁光介质夹层较厚的结构具有膜层数目少、工作稳定性好的优点.
关键词:
光隔离器
磁光效应
一维光子晶体 相似文献
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采用4×4传输矩阵法研究了两种结构一维磁光子晶体的光隔离特性.结构一在外加磁场与光路光轴方向呈52.0°时,用7.96μm的总厚度在中心波长附近0.95nm范围内实现了光隔离,在此范围之内法拉第旋转角和透射率分别在45°~50.65°和97.01%~99.96%之间波动,结构仅包含43层光学薄膜,易于实际制备;结构二在外加磁场与光路光轴方向呈32.7°时,用11.54μm的总厚度在中心波长附近0.85nm范围内实现了光隔离,在此范围之内法拉第旋转角和透射率分别在45°~48.55°和98.85%~100%之间波动,结构包含73层光学薄膜,与结构一相比,该结构具有更高的透射率和更平坦的光谱.用这两种结构的一维磁光子晶体代替目前商用磁光隔离器中的块状磁光介质,可实现磁光隔离器的集成化. 相似文献
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一维光子晶体带隙结构研究 总被引:28,自引:6,他引:22
在考虑介质色散的基础上,研究了介质层厚度对光子晶体带隙结构的影响.利用传输矩阵法,计算了以LiF和Si两种材料组成的一维光子晶体带隙结构.结果表明,介质层厚度的增加会引起禁带的红移,厚度减小会引起蓝移.分析了含空气缺陷层、金属缺陷层的光子晶体结构,发现空气缺陷层对带隙结构的高反射区域变化不大,而在低反射区域,反射系数为零的波带之间出现了两边反射系数增加,中间反射系数减小的情况.在金属缺陷层的带隙结构中,金属对整个波长范围光的吸收作用不同,金属对低反射区1.6 μm、1.85 μm处透射率较大的透射光吸收作用明显,而在1.28~1.38 μm处透射率波长区间,几乎无吸收. 相似文献
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基于平面波展开法,设计三层一维光子晶体横磁场模结构,改变三层介质厚度和介质折射率的大小,应用MATLAB语言进行仿真计算,在一维光子晶体三层介质厚度值为0.4、0.05μm和0.05μm,折射率为1、3N和12N时形成一维光子晶体带隙宽度最宽为0.2694Hz.研究结论为一维光子晶体器件的设计提供理论依据. 相似文献
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结合干涉光刻和磁控溅射制备了一维周期性起伏的磁性多层薄膜。利用扫描探针显微镜对样品的微结构进行表征,利用椭偏仪和磁光测量系统对样品的光学性能参数和磁光克尔效应进行测试和研究。实验结果发现,磁性多层薄膜磁光性能得到极大的提升,磁光增强的克尔谱峰值与条带的宽度、中间层二氧化铪层的厚度有关;利用介质层的厚度可调制复合薄膜的磁光特性。进一步研究发现横克尔效应的增强现象。理论计算的结果证实,磁光增强源于光学腔干涉共振和磁等离激元的耦合效应。 相似文献
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利用掺杂浓度为5 mol%的掺氧化镁多周期极化铌酸锂晶体实现了高效单谐振的准相位匹配光参量振荡器,所使用的周期极化铌酸锂晶体有6个周期,且以1 μm为间隔,从26.5~31.5 μm. 该光参量振荡器以脉宽为150 ns,重复频率为10 kHz的声光调Q Nd∶YAG激光器为泵浦源,且泵浦光波长为1.064 μm. 通过控制晶体的温度(50~200℃)以及改变晶体的极化周期(26.5~31.5 μm),可由该光参量振荡器获得2.83~2.89 μm,3.10~3.38 μm,3.57~3.78 μm,3.95~4.12 μm, 4.28~4.46 μm,4.65~4.79 μm的闲频光连续调谐输出. 且当泵浦功率为8.15 W时,在闲频光输出波长为3.33 μm处,获得了最大输出功率2.17 W. 相似文献
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用特征矩阵法研究了带缺陷的一维光子晶体的透射性质,并提出了新的可调谐光滤波器的概念.一维光子晶体(L1H1)m带有Lc-H2(L2H2)n形式的缺陷时,在光子晶体中间出现了窄的透射峰,其他级次的干涉峰则随着覆盖层H2(L2H2)n周期数的增大而减弱并消失.当耦合层Lc厚度变化时,在光子晶体禁带边缘附近出现两个高透射率区域.高透射率区域透射峰的特性由光子晶体和覆盖层的性质决定.当光子晶体禁带宽度较小时,两个高透射率区域接近,形成具有约150nm调谐范围的区域,因此可制备以一维光子晶体为基础的新型可调谐光滤波器.
关键词:
光子晶体
可调谐光滤波器
特征矩阵 相似文献
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V.A. Kosobukin 《Solid State Communications》2006,139(3):92-96
A theory is presented for propagation of electromagnetic waves through one-dimensional magnetic Bragg structures (magneto-photonic crystals). Within the self-consistent Green-function technique the transfer matrices and magneto-optical characteristics are derived in terms of circularly polarized waves propagating in periodical arrays of alternating magnetic and dielectric layers. For finite-thickness magneto-photonic crystals, the Faraday rotation and other magneto-optical responses are demonstrated to change considerably in the spectral range of stop-bands, the magnetic modulation of the in-plane reflection intensity being essentially enhanced. 相似文献
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Specific features of the energy-band structure of magneto-photonic crystals have been studied. The problem of the propagation of light through a finite layer of a magneto-photonic crystal has been solved by the modified Ambartsumyan layer-summation method. The effect of the direction of an external magnetic field on the band structure has been studied in detail and shown to alter the number of forbidden bands, change the frequency widths of these bands, and modify their polarization-related properties. Such systems have been shown to possess four eigenpolarizations. 相似文献
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Mathieu Francoeur M. Pinar Mengü Rodolphe Vaillon 《Journal of Quantitative Spectroscopy & Radiative Transfer》2009,110(18):2002-2018
A general algorithm is introduced for the analysis of near-field radiative heat transfer in one-dimensional multi-layered structures. The method is based on the solution of dyadic Green's functions, where the amplitude of the fields in each layer is calculated via a scattering matrix approach. Several tests are presented where cubic boron nitride is used in the simulations. It is shown that a film emitter thicker than 1 μm provides the same spectral distribution of near-field radiative flux as obtained from a bulk emitter. Further simulations have pointed out that the presence of a body in close proximity to an emitter can alter the near-field spectrum emitted. This algorithm can be employed to study thermal one-dimensional layered media and photonic crystals in the near-field in order to design radiators optimizing the performances of nanoscale-gap thermophotovoltaic power generators. 相似文献
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V. A. Tolmachev 《Optics and Spectroscopy》2017,122(4):646-660
The theoretical and experimental investigations of photonic band gaps in one-dimensional photonic crystals created by micromatchining silicon, which have been performed by the author as part of his doctoral dissertation, are presented. The most important result of the work is the development of a method of modeling photonic crystals based on photonic band gap maps plotted in structure–property coordinates, which can be used with any optical materials and in any region of electromagnetic radiation, and also for nonperiodic structures. This method made it possible to realize the targeted control of the optical contrast of photonic crystals and to predict the optical properties of optical heterostructures and three-component and composite photonic crystals. The theoretical findings were experimentally implemented using methods of micromatchining silicon, which can be incorporated into modern technological lines for the production of microchips. In the IR spectra of a designed and a fabricated optical heterostructure (a composite photonic crystal), extended bands with high reflectivities were obtained. In a Si-based three-component photonic crystal, broad transmission bands and photonic band gaps in the middle IR region have been predicted and experimentally demonstrated for the first time. Si–liquid crystal periodic structures with electric-field tunable photonic band-gap edges have been investigated. The one-dimensional photonic crystals developed based on micromatchining silicon can serve as a basis for creating components of optical processors, as well as highly sensitive chemical and biological sensors in a wide region of the IR spectrum (from 1 to 20 μm) for lab-on-a-chip applications. 相似文献
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A.M. Merzlikin A.P. Vinogradov M. Inoue A.B. Khanikaev A.B. Granovsky 《Journal of magnetism and magnetic materials》2006
The necessary conditions for the observation of the Faraday effect in 2D magneto-photonic crystals are discussed. It is found. that the Faraday effect may be observed in the directions where any couple of the wave vectors of the harmonics consisting the Bloch waves of TE and TM solutions in zero magnetic field are identical. This direction corresponds neither to Faraday nor to Voigt geometry. 相似文献
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《中国光学快报(英文版)》2017,(11)
A novel H-plane cross-shaped circulator based on magneto-photonic crystals is experimentally investigated.The band gap of the TE mode for the photonic crystals is calculated by the plane wave expansion method.The transmission characteristics of the circulator are simulated by the finite element method.We perform the experiments in the microwave regime to validate the numerical results.At the central frequency of 10.15 GHz,the measured isolation and insertion loss of the circulator reaches-30.2 and-3.93 d B,respectively.The bandwidth of the circulator is about 550 MHz.The optimal experimental value of isolation is higher than the numerical value. 相似文献
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填充率渐变型波状结构二维光子晶体 总被引:6,自引:2,他引:4
填充率渐变引起的能带结构和等频面结构的变化是填充率渐变型波状结构二维(2D)光子晶体(PC)产生光路转弯现象的根本原因,由于TM模和TE模在能带结构上存在差异,光路转弯现象就具有明显的偏振选择特性,能够实现归一化频率a/λ为0.29~0.33的偏振分束。利用时域有限差分(FDTD)法模拟了TM模的U型转弯波导,发现出射光位置对入射波长和入射角的变化很敏感,位移变化量分别达到0.38μm/10 nm和0.29μm/(°)。利用TM模的U型转弯波导构建了新型的平行平面谐振腔,并指出由填充率渐变型波状结构二维光子晶体和一维多层薄膜构成的混合结构在光分束和抑制光束发散方面的作用及其在平行平面谐振腔中的潜在应用。 相似文献
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ZnO/AlN/Si(111)薄膜的外延生长和性能研究 总被引:2,自引:0,他引:2
用常压金属化学气相沉积法(MOCVD)在Si(111)衬底上制备了马赛克结构ZnO单晶薄膜。引入低温Al N缓冲层以阻止衬底氧化、缓解热失配和晶格失配。薄膜双晶X射线衍射2θ/ω联动扫描只出现了Si(111)、ZnO(000l)及Al N(000l)的衍射峰。ZnO/Al N/Si(111)薄膜C方向晶格常量为0.5195nm,表明在面方向处于张应力状态;其对称(0002)面和斜对称(1012)面的双晶X射线衍ω摇摆曲线半峰全宽分别为460″和1105″;干涉显微镜观察其表面有微裂纹,裂纹密度为20cm-1;3μm×3μm范围的原子力显微镜均方根粗糙度为1.5nm;激光实时监测曲线表明薄膜为准二维生长,生长速率4.3μm/h。低温10K光致发光光谱观察到了薄膜的自由激子、束缚激子发射及它们的声子伴线。所有结果表明,采用金属化学气相沉积法并引入Al N为缓冲层能有效提高Si(111)衬底上ZnO薄膜的质量。 相似文献