紧凑型L波段磁绝缘线振荡器的实验设计

 设计加工了一个L波段磁绝缘线振荡器(MILO)，并进行了实验研究。在二极管电压为515~538kV, 二极管电流为58~61kA的条件下, 获得了频率为1.76~1.78GHz，功率为2.2~2.5GW的TM₀₁模高功率微波辐射, 功率转换效率为7.3%~7.9%。实验结果与模拟结果符合得较好。     

L波段双阶梯阴极磁绝缘线振荡器的粒子模拟与实验研究

对L波段双阶梯阴极磁绝缘线振荡器(MILO)进行了粒子模拟,在输入电压710 kV,电流56.6kA条件下,得到微波输出功率为4.8 GW,微波频率1.22 GHz。根据模拟结果设计MILO实验装置并开展实验研究,介绍了测试方法与测试系统,并对辐射微波功率、频率和模式进行了测量。在二极管电压740 kV,电流61 kA条件下,测得辐射微波功率为3.57 GW,微波脉宽46 ns,微波频率1.23 GHz,功率转换效率8%,辐射微波模式为TM01模。     

C波段磁绝缘线振荡器的理论设计与实验

 通过理论分析与计算，设计加工了一个C波段磁绝缘线振荡器（MILO），并进行了实验研究。在二极管电压为437～464 kV、二极管电流为36～39 kA的条件下，从实验上获得了功率为1.60～1.68 GW、频率为3.60～3.66 GHz、脉宽为33～38 ns的TEM模高功率微波辐射，功率转换效率大于9%。     

L波段硬管磁绝缘线振荡器的研制

 对L波段磁绝缘线振荡器(MILO)的二极管进行了研究，优化了器件的设计，以及辐射天线一体化的设计，研制出了L波段硬管 MILO。硬管MILO的实验结果是：在电压为450 kV、电流为35 kA的条件下，L波段硬管 MILO的输出微波频率为1.22 GHz，功率大于1.5 GW，微波脉宽半高宽约20 ns，功率效率约10%；硬管MILO的保真空时间超过了5 h。     

阶梯阴极型L波段MILO的实验研究

 对阶梯阴极型L波段磁绝缘线振荡器（MILO）进行了实验研究。介绍了测试方法与测试系统；开展了阴极电子发射实验，发现阴极电子发射不均匀是对称结构MILO产生非对称微波模式的最关键的因素之一；并对二极管屏蔽环尺寸、扼流片半径、提取间隙等进行了研究。在电子束电压约420 kV、电流33 kA的条件下，得到了阶梯阴极型L波段MILO的高功率微波辐射功率为1.22~1.47 GW，脉宽大于20 ns，频率为1.21 GHz，束波转换效率约为10%，器件产生微波模式为TM01模，经过模式转换器后的辐射模式为TE11模。     

重复频率X波段类周期加载微波腔的实验研究

在CHP-01加速器上对我所提出的X波段类周期加载微波腔进行了实验研究. 在实验中,首先对加速器进行了调试,使其能够稳定运行;然后对磁场、电压等参数与微波输出的关系进行了研究; 最后在二极管电压约为790kV、电流约为6.7kA时得到了微波输出功率为1.4GW、微波频率为9.4GHz、微波脉宽为30ns、束波转换效率为26%的实验结果.     

HEM11模磁绝缘线振荡器的高频分析

作为小型化和紧凑型的高功率微波源,磁绝缘线振荡器(MILO)在过去十几年里得到了广泛的研究和发展.在大多数研究中,最低的对称模一直被当作器件的主模.然而,由于结构的对称性或者电子发射均匀度不理想等原因,很容易激励起非对称模式.计算了MILO同轴结构中同时包含对称模和非对称模的本征方程.在此基础上,通过对结构的优化设计,提出了一种HEM..模工作的MILO,并开展了原理性实验.在二极管的电压为480 kV,电流为39kA条件下得到了功率为1.2 GW,脉冲宽度为加40 ns 的微波输出,功率转换效率约为6.5%,微波频率为1.98 GHz,模式为HEM11模.     

重复脉冲强流电子束源长时间稳定运行实验研究

 简要阐述了脉冲变压器型重复脉冲强流电子束加速器CHP01的组成、主要特点及工作原理，利用设计的重复脉冲强流电子束源进行了长时间运行实验研究，实验结果达到：在100 Hz重复频率下连续运行5 s，脉冲变压器能稳定输出电压1.15 MV,强流束二极管输出电压超过800 kV、束流7 kA、脉冲宽度45 ns，阴极电子发射密度超过10 kA/cm²，且运行稳定可靠。利用该电子束源进行了X波段类周期慢波结构微波器件实验研究，在50 Hz重复频率下连续运行5 s，输出微波功率超过1 GW，脉冲宽度大于25 ns。     

低阻抗紧凑型Marx直接驱动高功率微波源北大核心CSCD

研制了一套紧凑型脉冲功率源系统,用于驱动低阻抗磁绝缘线振荡器(MILO)。脉冲功率源采用Marx发生器技术路线,由10级电容和开关组成,单级电容为100nF/100kV电容,开关采用环形轨道气体火花间隙开关,通过紧凑型结构设计,降低系统回路电感,采用电阻作为级间放电的隔离元件,整个Marx发生器系统放置于变压器绝缘油中,以实现高压绝缘。Marx发生器系统充电电压为±50kV,总储能5kJ,在12Ω的水负载上可以获得600kV,50kA的脉冲输出,脉冲上升时间小于100ns。系统尺寸为1.2m×0.5m×0.6m。基于该低阻抗脉冲功率系统,直接驱动低阻抗磁绝缘线振荡器。在二极管电压约450kV,电流约40kA条件下,测得辐射微波功率约400MW,微波脉宽约60ns,微波频率1.23GHz,辐射微波模式为TM01模。     

L波段相对论返波振荡器初步实验研究

设计了一个紧凑型L波段相对论返波振荡器(RBWO),利用Karat 2.5维全电磁粒子模拟程序研究了器件内部束-波作用的物理过程。模拟结果表明:在二极管电压700 kV、电子束流10 kA、导引磁场为1.0 T时,能实现L波段2.23 GW高功率微波输出,平均效率约为31.8%。为验证模拟结果,在高阻加速器平台上进行了初步实验:当二极管电压为703 kV、电流10.6 kA、导引磁场为0.8 T时,实验获得了峰值功率1.05 GW、频率1.61 GHz、脉宽38 ns的高功率微波输出,其功率效率为14.4%。     

Investigation of an X-band magnetically insulated transmission line oscillator

An X-band magnetically insulated transmission line oscillator （MILO） is designed and investigated numerically and experimentally for the first time. The X-band MILO is optimized in detail with KARAT code. In simulation, the X-band MILO, driven by a 720 kV, 53 kA electron beam, comes to a nonlinear steady state in 4.0 ns. High-power microwaves （HPM） of TEM mode is generated with an average power of 4.1 GW, a frequency of 9.3 GHz, and power conversion efficiency of 10.870 in durations of 0-40 ns. The device is fabricated according to the simulation results. In experiments, when the voltage is 400 kV and the current is 50 kA, the radiated microwave power reaches about 110 MW and the dominating frequency is 9.7GHz. Because the surfaces of the cathode end and the beam dump are destroyed, the diode voltage cannot increase continuously. However, when the diode voltage is 400 kV, the average power output is obtained to be 700 MW in simulation. The impedance of the device is clearly smaller than the simulation prediction. Moreover, the duration of the microwave pulse is obviously shorter than that of the current pulse. The experimental results are greatly different from the simulation predictions. The preliminary analyses show that the generations of the anode plasma, the cathode flare and the anode flare are the essential cause for the remarkable deviation of the experimental results from the simulation predictions.     

A Ku-band magnetically insulated transmission line oscillator with overmoded slow-wave-structure

In order to enhance the power capacity, an improved Ku-band magnetically insulated transmission line oscillator(MILO) with overmoded slow-wave-structure(SWS) is proposed and investigated numerically and experimentally. The analysis of the dispersion relationship and the resonant curve of the cold test indicate that the device can operate at the near π mode of the TM01 mode, which is useful for mode selection and control. In the particle simulation, the improved Ku-band MILO generates a microwave with a power of 1.5 GW and a frequency of 12.3 GHz under an input voltage of480 k V and input current of 42 k A. Finally, experimental investigation of the improved Ku-band MILO is carried out. A high-power microwave(HPM) with an average power of 800 MW, a frequency of 12.35 GHz, and pulse width of 35 ns is generated under a diode voltage of 500 k V and beam current of 43 k A. The consistency between the experimental and simulated far-field radiation pattern confirms that the operating mode of the improved Ku-band MILO is well controlled inπ mode of the TM01 mode.     

HEM₁₁ mode magnetically insulated transmission line oscillator:Simulation and experiment

A novel magnetically insulated transmission line oscillator(MILO) in which a modified HEM 11 mode is taken as its main interaction mode(HEM 11 mode MILO) is simulated and experimented in this paper.The excitation of the oscillation mode is made possible by carefully adjusting the arrangement of each resonant cavity in a two-dimensional slow wave structure.The special feature of such a device is that in the slow-wave-structure region,the interaction mode is HEM 11 mode which is a TM-like one that could interact with electron beams effectively;and in the coaxial output region,the microwave mode is TE 11 mode which has a favourable field density pattern to be directly radiated.Employing an electron beam of about 441 kV and 39.7 kA,the HEM 11 mode MILO generates a high power microwave output of about 1.47 GW at 1.45 GHz in particle-in-cell simulation.The power conversion efficiency is about 8.4 % and the generated microwave is in a TE 11-like circular polarization mode.In a preliminary experiment investigation,high power microwave is detected from the device with a frequency of 1.46 GHz,an output energy of 43 J-47 J,and a pulse duration of 44 ns-49 ns when the input voltage is 430 kV-450 kV,and the diode current is 37 kA-39 kA.     

HEM11 mode magnetically insulated transmission[2mm] line oscillator: simulation and experiment

A novel magnetically insulated transmission line oscillator (MILO) in which a modified HEM₁₁ mode is taken as its main interaction mode (HEM₁₁ mode MILO) is simulated and experimented in this paper. The excitation of the oscillation mode is made possible by carefully adjusting the arrangement of each resonant cavity in a two-dimensional slow wave structure. The special feature of such a device is that in the slow-wave-structure region, the interaction mode is HEM₁₁ mode which is a TM-like one that could interact with electron beams effectively; and in the coaxial output region, the microwave mode is TE₁₁ mode which has a favourable field density pattern to be directly radiated. Employing an electron beam of about 441 kV and 39.7 kA, HEM₁₁ mode MILO generates a high power microwave output of about 1.47 GW at 1.45 GHz in particle-in-cell simulation. The power conversion efficiency is about 8.4 % and the generated microwave is in a TE₁₁-like circular polarization mode. In a preliminary experiment investigation, high power microwave is detected from the device with a frequency of 1.46 GHz, an output energy of 43 J-47 J, and a pulse duration of 44 ns-49 ns when the input voltage is 430 kV-450 kV, and the diode current is 37 kA-39 kA.     

HEM11模磁绝缘线振荡器的高频分析

作为小型化和紧凑型的高功率微波源,磁绝缘线振荡器(MILO)在过去十几年里得到了广泛的研究和发展.在大多数研究中,最低的对称模一直被当作器件的主模.然而,由于结构的对称性或者电子发射均匀度不理想等原因,很容易激励起非对称模式.计算了MILO同轴结构中同时包含对称模和非对称模的本征方程.在此基础上,通过对结构的优化设计,提出了一种HEM₁₁模工作的MILO,并开展了原理性实验.在二极管的电压为480kV,电流为39kA条件下得到了功率为1.2GW,脉冲宽度为40ns的微波输出,功率转换 关键词： 磁绝缘线振荡器 高频特性 11模')" href="#">HEM₁₁模 开放腔     

折叠型平板Blumlein线高功率微波驱动源

 介绍了一种使用折叠型平板Blumlein线为主体的紧凑型高功率微波驱动源,Kapton薄膜和纯净变压器油分别作为折叠型平板Blumlein线的传输线介质和绝缘介质,Blumlein线的整体尺寸为1.00 m×0.40 m×0.15 m。采用一个特征阻抗大约是12 W的C波段磁绝缘振荡器作为高功率微波源。折叠型平板Blumlein线传输的能量可以使磁绝缘振荡器的阴极发射出电压550 kV,电流40 kA ,脉宽90 ns的电子束,从而产生峰值功率350 MW,脉宽40 ns的高功率微波。     

轴向分区双频磁绝缘线振荡器的数值模拟

 为了便于模式变换器的设计,达到双频微波都能集中辐射的目的,提出一种轴向分区的双频磁绝缘线振荡器,该器件束波互作用区为中间隔开、两端不同周期、不同深度的慢波结构,使电子在上下游与不同频率特性的慢波结构进行束波互作用,得到稳定的双频微波输出。使用2.5维全电磁粒子模拟软件进行数值模拟,在工作电压450 kV,电流40 kA条件下输出微波功率为1.4 GW,功率效率约为7%,输出的微波频率分别为1.25 GHz和1.65 GHz,两者频谱幅度相差约为1.5 dB,模式为TEM模。