传输可见光的空芯光子带隙光纤的研究

利用全矢量平面波展开法(FVPWM)对采用改进的两次堆积法制备的空芯光子带隙光纤进行了数值模拟.在特定传播常数β下,光纤在500—1000 nm的波段内出现多条宽窄不同的有效光子带隙.依据有效折射率的不同,部分带隙中的空气-导模将以不同的形式存在.经过实验测试,发现测得的带隙位置相对于模拟结果向短波段发生了较明显的移动,主要原因被认为是光纤结构的纵向不均匀性和包层节点处间隙孔的存在. 关键词： 空芯光子带隙光纤 全矢量平面波展开法 有效光子带隙 空气-导模     

光源偏振度对光纤陀螺零漂影响的研究

以Y波导集成光学调制器保偏型干涉式光纤陀螺作为研究对象,根据各光学元器件的参数建立了各器件的琼斯矩阵以及光路传输模型,在此基础上进行了光路偏振误差的理论分析。通过推导,得到了保偏型干涉式光纤陀螺的偏振误差表达式,并首次分析了光源偏振度对光纤陀螺零漂的影响。借助光源尾纤输出的光谱,对由0%~3%之间呈线性变化的偏振度以及对经实验测试的光源偏振度的实际值引起的偏振模式耦合误差的零漂值进行了仿真计算。结果表明,当光路中其它参数不变时,由光源偏振度变化引起的零漂值为0.001°/h,满足了高精度光纤陀螺的精度要求。     

单偏振控制器环形腔光纤激光器实验研究

理论分析了非线性偏振旋转环形腔作为类饱和可吸收体获得脉冲的物理机理。在光纤环形腔结构中,采用单个偏振控制器实现了非线性偏振旋转锁模,直接获得了脉冲宽度为131 fs的超短脉冲输出。实验中,采用性能稳定的976 nm半导体二极管激光器作为抽运源,使用高掺杂浓度的Er3 光纤为增益介质,通过调节偏振控制器,获得了光谱谱宽(3 dB带宽处)为23.5 nm的稳定锁模脉冲输出。脉冲中心波长为1535.9 nm,平均功率为5.91 mW,脉冲重复率为11.20 MHz。     

基于光纤SPR光谱分析的污水降解过程监测研究

讨论了光纤表面等离子体波传感器的工作原理,并对将其用于监测以甲基橙为代表的环境污水降解过程的可行性进行了探讨。用光纤SPR传感器监测了50 mL初始浓度为30 mg·L-1的甲基橙原溶液在降解过程浓度的变化,对降解过程中光纤SPR传感器的光谱进行了详细的分析;同时采用紫外-分光光度计对降解过程中溶液浓度的变化进行了监测,并对2种方法所测的数据进行了分析对比。结果表明,光纤SPR同常规方法的测量结果一致,随着降解时间的增加,甲基橙溶液的吸光度和浓度逐渐减小,光纤SPR传感器的共振波长逐渐发生蓝移,同初始标定的甲基橙原溶液共振光谱比较,说明甲基橙逐渐被降解,且在2 h内降解率达到73%,说明用光纤SPR传感器监测污水降解过程是完全可行的。研究结果不仅为环境污水降解过程提供了一种新的监测方法,同时促进了我国SPR传感技术与环保监测研究结合,为光纤SPR技术走向实用,并最终实现产业化积累了经验。     

980nm单模运转未镀增透膜光纤光栅激光器

提出了一种工艺简单的980nm未镀增透膜的光纤光栅外腔半导体激光器。首先从理论上分析了边模抑制比(SMSR)与激光二极管前表面反射率R2、外腔长Lext和激光二极管一光纤耦合效率之间的关系,得出边模抑制比随R2和Lext的增大而减小,而随着激光二极管一光纤的耦合效率的提高而增大。从计算结果中还可以看出,即使半导体激光器不镀增透膜(R2=0．3时)。在其它参量合适的情况下,边模抑制比仍可大于40dB。然后,对其进行实验验证。在半导体激光器未镀模的情况下,选择光纤光栅发射率为0．5,外腔长为12．5cm,输人电流为28．8mA(约为阈值电流的2．4倍)时,通过仔细调节恒温、恒流电路,实现了边模抑制比高于40dB的稳定的单纵模输出,外腔激光器的线宽优于1．6MHz。     

双偏振结构保偏光纤偏振器的研制

提出了保偏光纤偏振器的一种串联结构,即双偏振结构,报道了研制的结果。并通过对单偏振结构和双偏振结构器件测试结果的比较,得出双偏振结构的保偏光纤偏振器可使器件达到高消光比,并且有稳定的温度特性。     

High sensitivity dual core photonic crystal fiber sensor for simultaneous detection of two samples

The optical control ability of photonic crystal fiber (PCF) is a distinctive property suitable for improving sensing and plasma performance. This article proposes a dual-core D-channel PCF sensor that can detect two samples simultaneously, which effectively solves the problems of coating difficulty and low wavelength sensitivity. The PCF has four layers of air holes, which dramatically reduces the optical fiber loss and is more conducive to the application of sensors in actual production. In addition, by introducing dual cores on the upper and lower sides of the central air hole, reducing the spacing between the core and the gold nanolayer, a stronger evanescent field can be generated in the cladding air hole. The optical fiber sensor can detect the refractive index of two samples simultaneously with a maximum sensitivity of 21300 nm/RIU. To the best of our knowledge, the sensitivity achieved in this work is the highest sensitivity with the dual sample synchronous detection sensors. The detection range of the refraction index is 1.35-1.41, and the resolution of the sensor is 4.695×10^-6. Overall, the sensor will be suitable for medical detection, organic chemical sensing, analyte detection, and other fields.     

Tunable and highly sensitive temperature sensor based on graphene photonic crystal fiber

Optical fiber temperature sensors have been widely employed in enormous areas ranging from electric power industry, medical treatment, ocean dynamics to aerospace. Recently, graphene optical fiber temperature sensors attract tremendous attention for their merits of simple structure and direct power detecting ability. However, these sensors based on transfer techniques still have limitations in the relatively low sensitivity or distortion of the transmission characteristics, due to the unsuitable Fermi level of graphene and the destruction of fiber structure, respectively. Here, we propose a tunable and highly sensitive temperature sensor based on graphene photonic crystal fiber (Gr-PCF) with the non-destructive integration of graphene into the holes of PCF. This hybrid structure promises the intact fiber structure and transmission mode, which efficiently enhances the temperature detection ability of graphene. From our simulation, we find that the temperature sensitivity can be electrically tuned over four orders of magnitude and achieve up to ～ 3.34×10^-3 dB/(cm·℃) when the graphene Fermi level is ～ 35 meV higher than half the incident photon energy. Additionally, this sensitivity can be further improved by ～ 10 times through optimizing the PCF structure (such as the fiber hole diameter) to enhance the light-matter interaction. Our results provide a new way for the design of the highly sensitive temperature sensors and broaden applications in all-fiber optoelectronic devices.     

采用振荡-放大结构的声光调Q Nd:YAG激光器及光纤传输聚焦系统

研究了一种氪灯抽运的双Nd:YAG棒和声光调制器构成一级振荡加一级放大的声光调QNd:YAG激光器.动态激光平均输出功率最大达到169W,在重复频率1kHz时,测得脉宽70ns,峰值功率达到594kW.用芯径0.6mm的全石英光纤传输激光,并设计了一套聚焦光学系统,实现了大幅面的激光雕刻工作.     

基于多模干涉和长周期光纤光栅的温度及折射率同时测量

基于多模干涉理论和长周期光纤光栅(LPFG)的传感特性,提出了一种单模-多模-单模(SMS)结构与LPFG级联的光纤传感器,实现了温度和折射率的同时测量。实验结果表明,SMS结构的干涉谱和LPFG对温度和折射率具有不同响应灵敏度,其温度灵敏度分别为0.017nm/℃和0.060nm/℃;SMS结构对折射率不敏感,而LPFG的折射率灵敏度为-35.60nm/RIU(RIU为折射率单位)。因此利用敏感矩阵,实现对温度和折射率的同时测量,得到温度和折射率的最大测量误差分别为±0.59℃和±0.0013。该结构灵敏度高、结构简单,且不易受电磁等干扰。实验结果具有良好的线性度,在生物化学领域应用前景良好。