高功率脉冲光隔离器非线性及热效应分析

从理论上分析了脉冲情况下,磁光晶体横向温度梯度引起的光弹效应、消光比以及克尔效应对光隔离器隔离度的影响,并与连续入射情况进行了对比。结果表明:在平均功率相同的情况下,脉冲光束入射比连续光束入射情况隔离度更低;当平均功率较小时,消光比对隔离度的影响较大;当平均功率较大时,消光比对隔离度的影响有限,主要表现出光弹效应对隔离度的影响;当峰值功率密度较大时,克尔效应将显著降低隔离度,并且峰值功率密度越大,对隔离度的降低程度越大。     

偏振光学系统中相位延迟机理及其应用

为了实现偏振编码的自由空间量子密钥分发实验,研制了偏振保持的光机系统,并对该系统所采用的相位延迟传输机理及应用进行了研究,建立了偏振误码率在允许范围内的量子链路.首先,采用矩阵光学理论对偏振光的方位角、相位延迟与消光比的关系进行了介绍.接着,通过矩阵光学理论及实验验证了偏振光学系统的相位延迟线性叠加原理.然后,在相位延迟线性叠加原理的基础上,设计了一套偏振保持光学系统,并通过理论分析及实验验证了此系统具备良好的偏振保持效果.最后,将偏振保持光学系统的设计机理应用于量子通信光机系统的设计之中,并取得了良好的设计效果.实验结果表明:相位之间的相互抵消可以有效地进行偏振保持设计,最终设计的量子通信光机系统的偏振消光比优于500∶1.满足了自由空间量子通信实验中对偏振误码率的要求.     

布儒斯特角法测量金属薄膜折射率并解释不消光现象

根据布儒斯特角原理对磁控溅射的铜膜样品进行了折射率的测量,实验发现当p偏振光以布儒斯特角入射时,反射光并没有完全消光.从理论上、通过数值计算分别论证了金属薄膜折射率的虚部、薄膜界面多次反射等因素的影响,并与实验结果比对得到符合的结果.     

高功率脉冲光隔离器非线性及热效应分析

从理论上分析了脉冲情况下,磁光晶体横向温度梯度引起的光弹效应、消光比以及克尔效应对光隔离器隔离度的影响,并与连续入射情况进行了对比。结果表明：在平均功率相同的情况下,脉冲光束入射比连续光束入射情况隔离度更低;当平均功率较小时,消光比对隔离度的影响较大;当平均功率较大时,消光比对隔离度的影响有限,主要表现出光弹效应对隔离度的影响;当峰值功率密度较大时,克尔效应将显著降低隔离度,并且峰值功率密度越大,对隔离度的降低程度越大。     

利用光纤环形镜提高级联长周期光栅干涉谱消光比的理论和实验分析

对级联长周期光栅干涉谱的特性进行了理论模拟，得到了输出端加入光纤环形镜，可以将其干涉谱消光比提高为原来两倍的结论.实验结果与理论相符.加入光纤环形镜的确为提高级联长周期光栅干涉谱消光比的一种简单有效的方法.     

非对称Ag纳米线三聚体中的等离体子共振及级联效应

本文采用二维有限元方法,研究了由非对称半径及间距组成的银纳米线三聚体的等离子体共振以及异常的电场分布现象. 模拟结果显示,非对称银纳米线三聚体中存在亮模和暗模. 当亮模分布于两根半径较小的纳米线之间时,会导致在较大半径的两根纳米线间出现较高的场增强分布,说明级联效应被抑制. 相反,当两根半径较小的纳米线之间存在暗模时,较大的场增强存在于两根较小半径的纳米线间,此时所产生的级联效应得以实现.     

Dual-wavelength fiber grating laser in linear overlapping cavity

We report a switchable dual-wavelength fiber grating laser in linear overlapping cavity. The laser features two overlapping cavities sharing a single Yb-doped gain medium fiber and two sets of fiber Bragg gratings. A coiling fiber setup is inserted into the 1035 nm laser cavity. Given that the bending loss is inversely related to the bending radius, the cavity loss of 1035-nm can be modulated. Modulating the bending loss facilitates the switching of the fiber grating laser to a single-or dual-wavelength output at 1030 or 1035 nm and convenient tuning of the power ratio of the two wavelengths. An approximately 152.6-mW output power and up to 38-dB polarization extinction ratio are observed. The simultaneous lasing at I030 and 1035 nm is a qualified seeder source for amplification to high power scale and can be applied to difference frequency generation of a terahertz signal. This dual-wavelength fiber grating laser is a potential pump source for generating terahertz radiation using a novel approach.     

脉冲激光测距机性能综合测试技术

提出利用室外消光法与室内时序增益系数比检测相结合的方法进行激光测距机最大测程测试,利用精密光电延时与激光回波模拟技术相结合的方法实现对测距机测程范围、测距精度、选通范围及精度、距离分辨力等主要性能参数的室内模拟测试。对测试原理进行了论述,并对激光测距机的实验数据进行了分析。实验结果表明:利用所提出的综合测试技术可实现对脉冲激光测距机多个主要性能参数的准确测试,为客观评价激光测距机的性能提供了可靠的测量数据。     

90.4-W all-fiber single-frequency polarization-maintained 1083-nm MOPA laser employing ring-cavity single-frequency seed oscillator

A high-power all-fiber single-frequency polarization-maintained（PM）laser operating at 1 083 nm is demonstrated using a master oscillator power amplifier（MOPA）structure.The seed source of this MOPA laser system is an in-house-built ring-cavity fiber oscillator.Four-stage amplification configuration is employed, in which the maximal output power of the main amplifier is 90.4 W,corresponding to a conversion efficiency of 72.5%.The polarization extinction ratio of the output light is 13 dB.The amplified spontaneous emission is suppressed by a factor of over 25 dB,and no stimulated Brillouin scattering effect is observed when a large-mode-area and high absorption coefficient PM gain fiber is employed.     

High power linearly polarized Raman fiber laser at 1120 nm

An all-fiber linearly polarized Raman fiber laser at 1120 nm is demonstrated. With a 1 070-nm linearly polarized Yb-doped fiber laser as pump source, an output of up to 7.7 W at 1120 nm is obtained with an optical efficiency of 55%. The polarization extinction ratio of the linearly polarized Raman fiber is higher than 18 dB. A numerical simulation model is developed to determine the Raman coefficient of the gain fiber and to evaluate the laser performance. The spectral isolation between the Raman fiber laser and the pump fiber laser is determined to be necessary for further improvements of performance.