非线性包层多量子阱波导的TE波

给出用以分析非线性包层多量子阱波导ＴＥ模光学非线性与双稳性的理论公式与计算方法。指出用均方根等效折射率法解本征方程是有效的简化方法。用本文方法分析了模折射率对波导总功率的依赖关系,芯区功率与总功率之间的双稳性以及模场分布与模折射率的关系。讨论了波导参数对光学非线性、双稳性及模场的分布的影响。     

四种非矩形截面传感波导中的TE波和TM波

用保角变换将非矩形截面传感波导变换成等效矩形截面波导．给出计算等效矩形截面波导的TE模和TM模、电磁场、临界频率、波导壁电流、功率传输和衰减的公式．并给出4种非矩形传感截面波导数值计算的例子．     

星形光波导耦合器的耦合特性分析

根据TE0模光波导的本征场分布、瑞利索末菲标量衍射积分公式和激励源与光波导耦合的匹配效率公式,给出光波导端面衍射和耦合的归一化发射系数和接收系数计算公式,推导出光波导端面非接触耦合的耦合效率计算公式。光波导模场分布采用高斯函数近似表达,给出简洁的计算光波导端面非接触耦合的耦合效率函数表达式。最后,基于星形光波导耦合器结构参量的特点,将累加运算采用积分运算近似表达,给出星形光波导耦合器接收光波导总的接收效率与耦合器基本参量的关系,阐明了星形光波导耦合器的耦合特性。     

棱镜耦合法测量掺杂波导模折射率中的误差分析

讨论了棱镜耦合法测量离子交换掺Er-Yb平面光波导中传播模式的模折射率实验中的误差与不确定度,模折射率误差由耦合棱镜折射率与底角及同步入射角误差决定，得出了测量模折射率不确定度的传递公式,作为实例．用Ag^＋-Na^＋离子交换技术,在285℃下交换15min．得到了Er-Yb共掺磷酸盐玻璃平面波导，给出了波导模折射率（@632．8nm）及不确定度。     

梯形截面介质光波导的模吸收损耗

本文运用微分法由梯形截面介质光波导的近似模方程导出了模吸收损耗系数的公式.并结合计算实例进行了误差分析.     

离子交换玻璃波导折射率分布的确定

本文提出了由模折射率确定波导表面折射率的新方法,简化了White提出的公式,且可适用于任意折射率分布的平面光波导,具有普遍意义。分析结果表明,理论计算与实验测量相符合。     

非线性对称平板光波导TE模色散特性的近似计算

本文利用微扰法,导出了克尔型非线性对称平板光波导TE模传播常数的近似计算公式。结果表明,本文公式得到的结果与精确结果吻合得很好。     

扇形波导谐振宽边纵缝的归一化电导

扇形波导可作为高功率微波圆柱共形波导缝隙阵天线的基本单元。分析了扇形波导中主模场分量,根据实际情况对主模场进行了合理近似。采用互易定理推导由波导主模横向场分量和缝隙场分量表示的波导场分量的前向或后向散射系数。根据波导传输线理论,将波导宽边纵缝等效为并联导纳,再根据波导边界条件得到扇形波导宽边谐振纵缝的归一化电导与波导散射系数之间的关系式。根据缝隙天线与振子天线的互补关系得到扇形波导谐振缝隙的辐射阻抗,结合波导功率平衡关系得到由波导横向场散射系数表示的缝隙辐射功率表达式,得到归一化电导的与谐振宽边纵缝的偏移位置、缝隙宽度、波导波长以及扇形波导尺寸参数之间的解析表达式。给出了算例,在波导中间区域,通过商用软件计算得到的电导与理论公式结果基本吻合。     

高斯分布扩散光波导折射率分布的多项式近似

本文用适当的多项式函数近似高斯折射率分布函数,利用Ikuno的结果,导出了扩散平面光波导导模有效折射率的更精确近似解公式.这个公式不仅简单便于计算,而且由它求得的导模有效折射率更接近光线方法的数值结果,其精度不仅优于无微扰的适当双曲正割分布近似,也优于微扰的适当双曲正割分布近似.同时也改善了较高阶导模的数据精度.     

磁诱导三维拓扑绝缘体波导中的导模

在三维拓扑绝缘体表面上外加铁磁条形成的磁势垒量子阱,通过控制入射电子能量,使得入射电子波限制在势阱中传播,并由波函数的连续性求得磁诱导三维拓扑绝缘体波导的色散方程.由于此方程是超越方程,不能解析求解,因此本文采用图解法求解色散方程的解,研究表明:在入射电子能量大于磁势垒和小于磁势垒的情况下,都能够形成波导;当入射电子的能量大于磁矢势时,波导能够支持基模,而且模式阶数也依次递增;而当入射电子能量小于磁矢势时,波导能够承载的导模数量有所减少.通过研究波导中导模几率密度的空间分布,发现三维拓扑绝缘体表面上磁场诱导的电子波导能够很好地束缚电子,而且低阶模对电子的束缚能力强于高阶模.此外,本文也推导出了波导的几率流密度分布的公式.     

用于太赫兹波传输的低损耗、高双折射光纤研究

提出了一种同时具有低吸收损耗、高双折射特性的新型太赫兹传输光纤.光纤由层状的聚四氟乙烯和空气层组成.采用有限元法分析了光纤的结构参数对其吸收损耗和双折射的影响.结果表明:这种光纤的双折射可高达0.08;在保证模式的吸收损耗小于20 dB/m的前提下,其双折射仍可大于0.02. 关键词： 太赫兹传输 吸收损耗 双折射 有限元法     

Loss measurements in graded-index compound-glass fibers

The optical fiber scattering loss coefficient is measured directly in a scattering sphere or deduced indirectly from total loss measurements. The results show agreement for graded-index silica-based fibers, but they seem conflicting for graded-index compound-glass fibers. This is explained from the diffusion-controlled refractive index profile and the ensuing mode-dependent scattering and absorption loss due to the different optical properties of core and cladding glass. Using this model the two-lengths total loss measurement method is discussed. A detailed experiment is described that convincingly illustrates the mode of operation of the scattering sphere as used in daily practice. The wavelength-independent term in the total loss, different for fibers drawn from the same glass, is explained as being scattering partly due to 1-mode mixing of modes with the same β by imperfections that affect high-1-modes predominantly. The total loss of the glasses to be investigated can be measured using low NA excited silicone-clad fibers and safely can be decomposed into scattering and absorption contributions.     

TM mode optical characteristics of five-layer MOS optical waveguides

The field distribution and complex eigenvalue equation of the TM mode are solved from the wave equation for a five-layer optical waveguide with finite metal cladding and a dielectric buffer layer. For air–Au–SiO₂–GaAs–AlGaAs MOS waveguides, numerical results for the propagation constant and absorption loss of the TM mode are computed in the complex plane from the eigenvalue equation. The effects of some guided structural parameters on the mode propagation and absorption loss are analysed and discussed.     

Loss measurements in graded-index compound-glass fibers

The optical fiber scattering loss coefficient is measured directly in a scattering sphere or deduced indirectly from total loss measurements. The results show agreement for graded-index silica-based fibers, but they seem conflicting for graded-index compound-glass fibers. This is explained from the diffusion-controlled refractive index profile and the ensuing mode-dependent scattering and absorption loss due to the different optical properties of core and cladding glass. Using this model the two-lengths total loss measurement method is discussed. A detailed experiment is described that convincingly illustrates the mode of operation of the scattering sphere as used in daily practice. The wavelength-independent term in the total loss, different for fibers drawn from the same glass, is explained as being scattering partly due to 1-mode mixing of modes with the same β by imperfections that affect high-1-modes predominantly. The total loss of the glasses to be investigated can be measured using low NA excited silicone-clad fibers and safely can be decomposed into scattering and absorption contributions.     

Measurement of the optical absorption coefficient for liquid based on optical microfiber

An inline measuring method of the optical absorption coefficient for liquid based on optical microfiber (OM) is studied. If an OM is immersed into absorptive liquid, the additional loss of the OM will increase. We have analyzed the relationship between the additional loss of the OMs and the absorption coefficients of the liquids, and found that the OM with determinate construction will be useful for measuring the absorption coefficients of the liquid whose refractive index is lower than that of the OM. Two OM samples are prepared to measure the absorption coefficient of pure water. A supercontinuum source is launched into the OM sample which is immersed into pure water, and absorption spectrum from 1400 to 1700 nm has been achieved by monitoring the additional loss. The trend of the absorption spectrum is similar with that of the reported result, showing that the inline measurement of the optical absorption coefficient is a feasible method for those lower refractive index liquids.     

掺Er3+光纤的γ射线辐射特性

本文研究掺Er³⁺光纤的γ射线辐射特性,发现在800到1600nm之间损耗都有显著的增加,有的增加800倍之多。光纤的γ射线辐照损耗特性具有β射线辐照类似的规律性。用γ射线的康普顿效应半定量地解释了这种类似性。对γ射线辐照损耗进行紫外线UV漂白,表明比热退火有更好的效果,能使损耗恢复50%。指出选用原子序数小的元素作光纤掺杂剂会有利于光纤抗辐照性能的提高。 关键词：     

双层孔大模场微结构光纤的模式特性分析

本文分析一种由两层低折射率孔组成的大模场光纤的模式特性.采用多极法和有限元方法数值计算并分析了内层孔与外层孔尺寸变化对光纤基模与高阶模的束缚损耗与弯曲损耗的影响,设计获得了一种具有较高的高阶模和基模损耗比同时允许一定程度弯曲的大模场光纤.结果表明:当内层孔直径为34 μm,外层孔直径为24 μm时,其基模束缚损耗为0.000 17 dB/m,而高阶模束缚损耗为1.39 dB/m;光纤的基模模场面积为2 150.9 μm²,当弯曲半径为1.2 m时,弯曲损耗为0.106 dB/m.     

石英光纤γ辐照损伤及其对近红外导波特性的影响

围绕光纤陀螺的近红外工作波长,从回波损耗、偏振相关损耗、散射损耗、吸收损耗、模场分布以及导模传播常数等方面实验考察了总剂量为120krad(1.2kGy)的γ辐照对石英单模光纤导波特性的影响;用近红外光谱技术和受激喇曼散射实验估计了相应的隙内缺陷能级及其增量;用X衍射考察了介质密度变动;采用高灵敏度干涉回路观察到了γ辐照光纤的光热效应,测试数据表明紫外退火具有一定的修复作用,揭示了紫外退火作为一种主动加固方式用于抗γ辐照的可能性.     

A novel coupled quantum well structure and its excellent electro-optical properties

A novel InGaAs/InAlAs coupled quantum well structure is proposed for large field-induced refractive index change with low absorption loss. In the case of low applied electric field of 15 kV/cm and low absorption loss (α≤ 100 cm-1), a large field-induced refractive index change (for transverse electric (TE) mode, △n = 0.012; for transverse magnetic (TM) mode, △n = 0.0126) is obtained in the structure at the operation wavelength of 1.55 μm. The value is larger by over one order of magnitude than that in a rectangular quantum well. The result is very attractive for semiconductor optical switching devices.