Hongxing Yang 1,2Yan Wang 1,2Ziqi Yin 1,2Pengcheng Hu 1,2,*[ ... ]Jing Li 1,2
Author Affiliations
Abstract
1 Center of Ultra-precision Optoelectronic Instrument, Harbin Institute of Technology, Harbin 150080, China
2 Key Laboratory of Ultra-precision Intelligent Instrumentation (Harbin Institute of Technology), Ministry of Industry and Information Technology, Harbin 150080, China
To ensure the frequency accuracy of a heterodyne laser source in the ambient temperature range of -20°C to 40°C, a dual-longitudinal-mode thermally stabilized He–Ne laser based on non-equilibrium power locking was designed. The ambient adaptive preheating temperature setting scheme ensured the laser could operate normally in the range of -20°C to 40°C. The non-equilibrium power-locked frequency stabilization scheme compensated for the frequency drift caused by different stabilization temperatures. The experimental results indicated that the frequency accuracy of the laser designed in this study could reach 5.2 × 10-9 in the range of -20°C to 40°C.
He–Ne laser frequency accuracy ambient adaptability non-equilibrium power locking 
Chinese Optics Letters
2024, 22(4): 041407
作者单位
摘要
西安交通大学 核科学与技术学院西安 710049
为研究兆瓦级高效紧凑型核动力系统的运行特性,使用自主开发的热管堆瞬态分析程序TAPIRS(Transient Analysis code for heat Pipe and AMTEC power conversion space Reactor power System)和超临界二氧化碳布雷顿循环的瞬态分析程序SCTRAN/CO2(Super Critical reactors Transient Analysis code/Carbon Dioxide)的耦合程序对其反应性、负荷、冷却水温度和流量等扰动进行了开环动态响应分析,并据此进行了控制系统设计。在此基础上,对线性变负荷、阶梯式变负荷以及甩负荷这三种变负荷运行工况进行了计算分析。结果表明:该核动力系统的转速对扰动的变化较为敏感,需要加以控制;低负荷下旁通会使压缩机流量上升,需对压缩机流量加以控制;系统在控制方案下能以6% FP(Full Power)·min-1的速度实现0%?100%的负荷变动,且可以在任意负荷水平下运行;甩负荷下系统的波动时间变长,但是仍可达到新的稳态进行工作,且各参数处于安全范围内。本研究可为新型核动力系统的概念设计提供参考。
兆瓦级高效紧凑新型核动力系统 开环动态响应 控制系统设计 变负荷运行 New megawatt nuclear power system with high efficiency and compactness Open-loop dynamic characteristics Design of control system Load variation operation 
核技术
2024, 47(2): 020601
Author Affiliations
Abstract
1 National Engineering Research Center for Optoelectronic Devices, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
2 College of Materials Sciences and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing 100049, China
The 975 nm multimode diode lasers with high-order surface Bragg diffraction gratings have been simulated and calculated using the 2D finite difference time domain (FDTD) algorithm and the scattering matrix method (SMM). The periods and etch depth of the grating parameters have been optimized. A board area laser diode (BA-LD) with high-order diffraction gratings has been designed and fabricated. At output powers up to 10.5 W, the measured spectral width of full width at half maximum (FWHM) is less than 0.5 nm. The results demonstrate that the designed high-order surface gratings can effectively narrow the spectral width of multimode semiconductor lasers at high output power.
laser diodes distributed Bragg reflector high order gratings high power laser diodes narrow spectrum width 
Journal of Semiconductors
2024, 45(3): 032401
作者单位
摘要
国防科技大学 电子科学学院,长沙 410076
随着电磁环境的日益复杂,电子设备面临的电磁威胁愈加严峻。光电系统作为高灵敏集成化电子设备,强电磁脉冲能量耦合进入系统内部,影响防护能力本就薄弱的光电系统的正常运行。为明晰典型光电系统强电磁耦合过程,通过仿真分析不同强电磁辐照条件下筒型、侧窗型和多窗口型三种典型光电系统的强电磁耦合情况,提取了光电系统强电磁耦合特征及其制约因素,验证了光电系统进行强电磁防护加固的必要性和紧迫性。为解决光电系统强电磁防护能力薄弱的问题,通过仿真分析,验证了透明电磁防护窗口的强电磁加固效能;开展了基于支撑台阶与导电侧壁的电磁缝隙防护加固方法研究,分析了透明防护窗口缝隙耦合泄露的关键安装结构参数,提出了一种非电接触式装配缝隙强电磁防护加固方法。经测试,当缝隙防护结构长度为6 mm时,在0.2~4 GHz频率范围光电系统平均强电磁防护效能提升4.51 dB。研究结果为光电系统强电磁防护能力提升提供了理论指导和具体解决方案。
光电系统 强电磁耦合分析 透明防护光窗 电磁防护方法 optoelectronic system high-power electromagnetic impulse coupling analysis transparent electromagnetic protection window electromagnetic protection method 
强激光与粒子束
2024, 36(4): 043010
作者单位
摘要
中国北方车辆研究所 电磁兼容试验室,北京 100072
电源变换系统中功率器件如MOSFET和IGBT开关管的高速切换将产生高幅值和宽频段的电磁干扰,是电动车辆最为常见也无法避免的电磁干扰源。同时,互连线缆是机电设备传递信号和能量的载体,是实现设备功能不可或缺的组成部分,线缆的天线效应使其成为设备产生电磁干扰的主要途径,是系统电磁兼容问题的主要根源之一。为了分析高压电源变换系统对低压控制系统的电磁耦合,以某典型地面装备电源变换系统IGBT开关管产生的脉冲宽度调制波(PWM波)作为电磁干扰源,以实装线缆作为分析对象,构建高低压线缆串扰模型,仿真分析不同线缆对地距离、线缆间距条件下单线、屏蔽线、双绞线等多类低压线缆的近端串扰电压,得出低压线缆的抗干扰性,为系统线缆的布线提供指导。
线缆 电磁兼容 电源变换系统 线缆串扰 共模干扰 cable harness electromagnetic compatibility power conversion system harness crosstalk common mode interference 
强激光与粒子束
2024, 36(4): 043023
作者单位
摘要
中国电子科技集团公司 第十二研究所,北京 100015
随着战场环境日益复杂,尤其是高对抗环境下,对现有各类装备均产生了极大威胁。设计了一款C波段雷达接收机保护器,采用充气微波开关管+波导同轴转换的结构设计,创新性地提出将固态限幅器芯片融合在波导同轴转换内部,限幅芯片采用级联的形式,提高了微带限幅器的承受功率。实现接收机保护器耐受功率10 MW以上,响应时间5 ns以内,不仅可用于雷达发射期间接收机防护,还可应对外部电磁干扰、高功率微波攻击。
复杂环境 高功率微波 电磁干扰 接收机保护器 微波等离子体 complex environment high-power microwave electromagnetic interference receiver protector microwave plasma 
强激光与粒子束
2024, 36(4): 043004
作者单位
摘要
1 国防科技大学 前沿交叉学科学院,长沙 410073
2 国防科技大学 理学院,长沙 410073
针对高功率微波波形参数对限幅器温度分布特性的影响,基于双级PIN限幅器的场路协同仿真模型对微波脉冲幅值、频率对温度分布的影响展开了仿真研究。结果表明:微波脉冲幅值、频率的提升会使双级PIN限幅器中PIN二极管的高温区域分布向P区拓展、高温区域分布范围扩大;相对而言,微波脉冲幅值对温度分布的影响更为显著,频率对温度分布的影响相对较小。
高功率微波 PIN限幅器 微波效应 热效应 温度分布 high power microwave PIN limiter microwave effect thermal effect temperature distribution 
强激光与粒子束
2024, 36(4): 043022
王晓阳 1,2滕飞 1,2,*徐小斌 3王琪伟 1,2[ ... ]李勇 1,2
作者单位
摘要
1 北京控制工程研究所,北京0090
2 空间智能控制技术重点实验室,北京100190
3 北京航空航天大学 仪器科学与光电工程学院,北京100191
光子带隙光纤有着独特的结构形式、传输介质和导光机制,这使其具有传统光纤无法比拟的优点,是未来光纤陀螺的理想选择。但光子带隙光纤粗糙的纤芯内壁导致其产生强烈的背向散射次波,会使光子带隙光纤陀螺产生额外的非互易误差。为了定量分析光子带隙光纤背向散射次波强度大小,论文基于电偶极子辐射理论建立了一种简单的光子带隙光纤背向散射次波理论模型。通过聚焦离子束微纳加工法和原子力显微镜测量得到了准确的纤芯内壁表面形貌功率谱密度,进而计算得到HC-1550-02型光子带隙光纤背向散射系数理论值为2.61×10-9/mm。通过光频域背向反射散射仪得到HC-1550-02型光子带隙光纤背向散射系数测量值为~1.82×10-9/mm,初步验证了背向散射次波模型的正确性,为背向散射次波抑制技术研究奠定了基础。
光子带隙光纤 背向散射次波 功率谱密度 photonic bandgap fiber backscatter secondary wave power spectral density 
光学 精密工程
2024, 32(6): 765
Yisha Chen 1,2,3Yun Ye 1,2,3Liangjin Huang 1,2,3,*Huan Yang 1,2,3[ ... ]Pu Zhou 1
Author Affiliations
Abstract
1 College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
2 Nanhu Laser Laboratory, National University of Defense Technology, Changsha 410073, China
3 Hunan Provincial Key Laboratory of High Energy Laser Technology, National University of Defense Technology, Changsha 410073, China
A low-numerical-aperture (NA) concept enables large-mode-area fiber with better single-mode operation ability, which is beneficial for transverse mode instability and nonlinear effects suppression. In this contribution, we reported a high-power fiber amplifier based on a piece of self-developed large-mode-area low-NA fiber with a core NA of 0.049 and a core/inner cladding diameter of 25/400 µm. The influence of the pump wavelength and fiber length on the power scaling potential of the fiber amplifier is systematically investigated. As a result, an output of 4.80 kW and a beam quality factor of ∼1.33 were finally obtained, which is the highest output power ever reported in a fiber amplifier exploiting the low-NA fiber. The results reveal that low-NA fibers have superiority in power scaling and beam quality maintenance at high power levels.
high power fiber lasers ytterbium-doped fiber low-numerical-aperture fiber mode instability 
Chinese Optics Letters
2024, 22(4): 041404
Author Affiliations
Abstract
1 School of Physics and Microelectronics, Zhengzhou University, Zhengzhou 450001, China
2 College of Physics Science and Technology, Institute of Applied Photonic Technology, Yangzhou University, Yangzhou 225002, China
The 1.4–1.8 µm eye-safe lasers have been widely used in the fields of laser medicine and laser detection and ranging. The diamond Raman lasers are capable of delivering excellent characteristics, such as good beam quality concomitantly with high output power. The intra-cavity diamond Raman lasers have the advantages of compactness and low Raman thresholds compared to the external-cavity Raman lasers. However, to date, the intra-cavity diamond cascaded Raman lasers in the spectral region of the eye-safe laser have an output power of only a few hundred milliwatts. A 1485 nm Nd:YVO4/diamond intra-cavity cascaded Raman laser is reported in this paper. The mode matching and stability of the cavity were optimally designed by a V-shaped folded cavity, which yielded an average output power of up to 2.2 W at a pulse repetition frequency of 50 kHz with a diode to second-Stokes conversion efficiency of 8.1%. Meanwhile, the pulse width of the second-Stokes laser was drastically reduced from 60 ns of the fundamental laser to 1.1 ns, which resulted in a high peak power of 40 kW. The device also exhibited single longitudinal mode with a narrow spectral width of < 0.02 nm.
diamond intra-cavity Raman lasers eye-safe lasers high peak-power 
Chinese Optics Letters
2024, 22(4): 041402

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