电调谐光纤布拉格反射滤波器

首次实现了采用磁致伸缩材料制作的电调谐光纤布拉格反射滤波器，实验得到１．３ｎｍ的调谐。滤波器带宽１．５ｎｍ。     

弱耦合光纤光栅外腔半导体激光器

报道作者对单频窄宽光纤光栅外腔半导体激光器的一些研究结果。理论上分析了外腔的引入对激光器的阈值增益和光谱线宽的影响，实验上用自行研制的光纤布拉格反射滤波器（ＦＢＲ）与普通多纵模半导体激光耦合，在１．５５μｍ波段，得到边模抑制比大于２５ｄＢ，线宽小于６０ｋＨｚ的激光输出。     

窄带高反射光纤布拉格反射滤波器

利用改进的非对称六层波导模型，分析了光纤布拉格反射滤波器的特性。讨论了波导结构参数－主要是高折射率层的厚度对器件特性的影响，指出了在制作过程中控制器件反射率的途径。     

基于侧边抛磨光纤的表面布拉格光栅温度传感器

为了实现在侧边抛磨光纤（SPF）上制作布拉格光栅结构并提高器件设计灵活性,利用重铬酸盐明胶（DCG）作为光刻材料,提出一种新型的光纤表面布拉格光栅制作方法并对该器件温度传感特性进行研究。使用轮式抛磨系统制作SPF,并在SPF侧抛面上旋涂DCG,通过干涉光束曝光显影制作表面布拉格光栅。光谱测量表明:带有布拉格光栅的侧边抛磨光纤在1 480.2 nm处有透射谷,在相应位置反射谱有明显反射峰,其调制幅度达到15.9 dB,这是由于表面光栅的布拉格反射所致。温度传感实验表明,该布拉格反射峰的温度灵敏度为17.84 pm/℃。这种器件已在光纤传感和光纤滤波器等方面获得应用。     

基于开槽型DBR光纤激光器拍频的折射率探测

提出一种包层开槽型分布布拉格反射光纤激光器,用于光纤激光折射率探测.该激光器以单纵模双偏振分布布拉格反射光纤激光器为核心传感单元,以结构双折射产生的拍频信号为传感信号对折射率进行探测.实验中应用频率编码,灵敏度高且易于解调.利用二氧化碳激光器的热效应对分布布拉格反射光纤激光器的谐振腔加工开槽,通过控制其扫描范围和功率来制备不同宽度和深度的开槽结构,并研究了不同结构参量对灵敏度特性的影响.实验测得最优灵敏度达-240 MHz/RI-unit.此外,还对该结构的温度传感特性做了测试,相较于未刻槽结构,温度灵敏度提高了21%,达1.73 MHz/℃.该装置结构紧凑、稳定性高、制备简单且成本低廉,可用于进一步研究分布布拉格反射光纤激光器的传感和复用特性.     

实现2.5 Gbit/s的波长变换

给出利用光注入分布布拉格反射激光二极管实现２．５Ｇｂｉｔ／ｓ的波长变换的实验结果。本结果实用于超高速光通信。     

利用光注入分布布拉格反射激光二极管实现2.5Gbit／s的波长变换

给出利用光注入分布布拉格反射激光二极管实现２．５Ｇｂｉｔ／ｓ的波长变换的实验结果。本结果实用于超高速光通信。     

用布拉格光纤光栅制作啁啾光纤光栅

介绍了一种用布拉格光纤光栅制作啁啾光纤光栅的方法。采用氢氟酸腐蚀布拉格光纤光栅, 使光栅的横截面沿光栅轴向逐渐变小, 然后对光栅施加１．５０ Ｎ的拉力, 在光栅轴向建立应变梯度, 制作出长１５ ｍ ｍ 、峰值反射率达９２％ 、反射半高宽为５ ｎｍ 的啁啾光纤光栅。     

用布拦格光纤光栅制作啁啾光纤光栅

介绍了一种用布拉格光纤光栅制作啁啾光纤光栅的方法。采用氢酸腐蚀布拉格光纤光栅,使光栅的横截面沿光栅轴向逐渐变小,然后对光栅施加１．５０Ｎ的拉力,在光栅轴向建立应变梯度,制作出长１５ｍｍ、峰值反射率达９２％、反射半高宽为５ｎｍ的啁啾光纤光栅。     

单频窄线宽分布布拉格反射光纤激光器研究

分析了单频窄线宽分布布拉格反射（DBR）光纤激光器的单模工作条件,在此基础上算出单模工作区域,制作了一个单频窄线宽分布布拉格反射光纤激光器。该激光器在波长为975.5nm的半导体激光器抽动下,在1556.91nm波长处。当抽运功率为55.35mW时输出功率可达1.43mW,频宽小于1.2MHz(受测量仪器分辨率限制）。经测量,该输出激光是稳定的单纵模输出。     

LaFeAsO单晶各向异性光学性质的第一性原理研究

使用密度泛函第一性原理研究了高温超导体LaFeAsO各向异性的光学性质。在描述光学性质的计算原理和计算方法的基础上, 计算了LaFeAsO的态密度、光电导谱、反射谱以及电子能量损失谱。光电导谱中, x方向与z方向有着很大差别, 在沿x方向的第一个带间吸收峰出现在1.3 eV处, 沿z方向出现在1.5 eV处; 在反射谱与电子能量损失谱中, x方向与z方向的特征峰位置在能量较高处都是相互吻合的。分析认为, 主要是电子在Fe原子之间的各个态间的跃迁所引起。考虑到温度效应对其光学性质的影响, 在计算光学矩阵元时, 加入Lorentz展宽δ=0.10 eV。本文的研究结果, 可为实验制备以及材料性质的研究提供有价值的参考。     

Experimental Study on Single Frequency Semiconductor Lasers with Fiber Bragg Reflector External Cavity

ＥｘｐｅｒｉｍｅｎｔａｌＳｔｕｄｙｏｎＳｉｎｇｌｅＦｒｅｑｕｅｎｃｙＳｅｍｉｃｏｎｄｕｃｔｏｒＬａｓｅｒｓｗｉｔｈＦｉｂｅｒＢｒａｇｇＲｅｆｌｅｃｔｏｒＥｘｔｅｒｎａｌＣａｖｉｔｙ￥ＡＮＨｏｎｇｌｉｎ；ＬＩＮＸｉａｎｇｚｈｉ；ＹＡＮＨｏｎｇ；ＣＵＩＸ...     

Optical evidence for a spin-filter effect in the charge transport of Eu0.6Ca0.4B6

We have measured the optical reflectivity R(omega) of Eu0.6Ca0.4B6 as a function of temperature (T) between 1.5 and 300 K and in external magnetic fields (H) up to 7 T. R(omega) increases with decreasing T and increasing H field, but the plasma edge feature does not exhibit the sharp onset and steep slope that is observed in EuB6. The analysis of the H-field dependence of the low-T optical conductivity confirms the previously observed exponential decrease of the electrical resistivity upon increasing bulk magnetization at constant T. The individual exponential magnetization dependences of the plasma frequency and scattering rate are also extracted from the optical data.     

High Reflection Ge_(0.45)Te_(0.55) Recording Films

ＨｉｇｈＲｅｆｌｅｃｔｉｏｎＧｅ０．４５Ｔｅ０．５５ＲｅｃｏｒｄｉｎｇＦｉｌｍｓＬＩＵＨｕｉｙｏｎｇＪＩＡＮＧＦｕｓｏｎｇＭＥＮＬｉｑｉｕＦＡＮＺｈｅｎｇｘｉｕＧＡＮＦｕｘｉ（ＳｈａｎｇｈａｉＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓ＆ＦｉｎｅＭｅｃｈａｎｉ...     

高光谱分辨率激光雷达鉴频器的设计与分析

提出了利用Fabry-Perot干涉仪的反射场实现高光谱分辨率激光雷达精细探测大气光学参量的新方法和思路.设计了高光谱分辨率的分光系统,并分析了干涉仪反射场的光谱透过特征曲线.结合高光谱激光雷达探测信号特征,讨论分析了谱分离比和瑞利信号透过率随反射率和腔长的变化曲线,同时结合误差传递公式,建立了仿真分析模型,讨论了回波光束发散角和入射角变化对激光雷达探测结果的影响.结果表明,所提出的Fabry-Perot干涉仪反射场可以实现高光谱分辨率激光雷达探测系统的精细分光,同时探测结果误差随回波光束发散角变化不敏感,控制发散角在10 mrad以内,入射角在1.5 mrad以内时,可以实现气溶胶光学参数廓线的高精度探测.     

光学击穿对受激布里渊散射特性的影响

把雪崩电离模型引入受激布里渊散射模型中，数值模拟了无光学击穿和有光学击穿时受激布里渊散射能量反射率随输入光功率密度的变化规律.实验上选取净化和未净化的CCl₄作为散射介质，在Nd:YAG调Q激光系统中进行了验证，理论与实验符合得很好.结果表明：当无光学击穿时，随着输入光功率密度的增大，能量反射率先是非线性增大，然后缓慢增大趋于饱和；而当有光学击穿时，随着输入光功率密度的增大，能量反射率先是非线性增大，达到最高值之后开始下降，最终趋于零.无光学击穿时的能量反射率及其稳定度明显高于有光学击穿时的情况. 关键词： 受激布里渊散射 光学击穿 雪崩电离     

Experimental investigation on the improvement of SBS characteristics by purifying the mediums

The influence of optical breakdown on stimulated Brillouin scattering (SBS) process is investigated with purified CCl4, acetone, and CS2 mediums which are obtained through 0.22-μm pore-size filter. Experiments are conducted with a Nd:YAG Q-switched laser system. The optical breakdown threshold, the reflectivity and the stability of SBS in both purified and unpurified mediums are determined and compared. The improvement of optical breakdown threshold is observed more or less in all purified mediums.In the condition that optical breakdown does not occur after the medium purified, the energy reflectivity and the stability of SBS both show improvement. Therefore, the characteristics of SBS can be improved by purifying the mediums to obtain higher optical breakdown threshold which reduces the influence of optical breakdown on SBS process.     

Short optical pulse generation from laser diodes with directional coupler external cavity

We demonstrate picosecond optical pulse (POP) generation from semiconductor laser diodes (LDs) operating in a novel external cavity configuration. The structure uses a looped directional coupler to form an optical cavity whose end reflectivity is controlled by the coupling constant. The end reflectivity can be varied continuously between 0 and 100%, and the cavity length can be adjusted by changing the loop length. A theoretical model and experimental verification of results on the generation of high-repetition POPS are presented.     

Reflectivity characteristics of the fiber loop mirror with a polarization controller

In this paper, reflectivity characteristics of a fiber loop mirror (FLM), which is formed by inserting a fiber polarization controller (PC) into the fiber loop of an ordinary FLM, are investigated in detail. A theoretical model for determining the reflectivity characteristics of the FLM is present by using the equivalent optical path technique, and the reflectivity characteristics of the FLM are then simulated with the model. The simulation results show that, when the FLM is based on a 3 dB optical coupler (OC), the reflectivity of the FLM may be continuously adjusted to any value between 1 and 0 by changing the PC state, i.e. by either changing the fast axis orientation or the birefringence intensity of the PC alone, as well as both of them; the reflectivity spectra of the FLM are wide and flattened for any PC state, mainly limited by the operating bandwidth of the OC used. The reflectivity characteristics of the FLM are further tested experimentally. The results verify that the reflectivity of the FLM may truly be continuously adjusted between its maximum and minimum values by changing the PC state. The obtainable maximum and minimum reflectivities of the FLM are measured to be 93% and 2%, respectively. Moreover, the experimental results are in agreement with those of the simulations.