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具有高稳定性的超高增益回旋行波管放大器

杜朝海 刘濮鲲 薛谦忠 徐寿喜 张世昌

杜朝海, 刘濮鲲, 薛谦忠, 徐寿喜, 张世昌. 具有高稳定性的超高增益回旋行波管放大器[J]. 电子与信息学报, 2010, 32(7): 1717-1720. doi: 10.3724/SP.J.1146.2009.00880
引用本文: 杜朝海, 刘濮鲲, 薛谦忠, 徐寿喜, 张世昌. 具有高稳定性的超高增益回旋行波管放大器[J]. 电子与信息学报, 2010, 32(7): 1717-1720. doi: 10.3724/SP.J.1146.2009.00880
Du Chao-hai, Liu Pu-kun, Xue Qian-zhong, Xu Shou-xi, Zhang Shi-chang. An Ultra-high Gain Gyrotron Traveling-Wave Amplifier with High Stability[J]. Journal of Electronics & Information Technology, 2010, 32(7): 1717-1720. doi: 10.3724/SP.J.1146.2009.00880
Citation: Du Chao-hai, Liu Pu-kun, Xue Qian-zhong, Xu Shou-xi, Zhang Shi-chang. An Ultra-high Gain Gyrotron Traveling-Wave Amplifier with High Stability[J]. Journal of Electronics & Information Technology, 2010, 32(7): 1717-1720. doi: 10.3724/SP.J.1146.2009.00880

具有高稳定性的超高增益回旋行波管放大器

doi: 10.3724/SP.J.1146.2009.00880

An Ultra-high Gain Gyrotron Traveling-Wave Amplifier with High Stability

  • 摘要: 该文结合线性理论和自洽非线性理论对Ka波段TE11模超高增益回旋行波管放大器的稳定性进行了研究。 研究揭示了回旋行波管中前向波绝对不稳定性和返向波振荡之间的区别,以及分布损耗技术对这两种自激振荡的抑制作用,并首次提出通过渐变磁场技术来提高系统的稳定性。基于该分析方法设计的Ka波段超高增益回旋行波管,采用电压100 kV,电流7 A,速度零散5%的电子注,获得了-1 dB的饱和功率带宽约5 GHz,最高增益约80 dB。
  • Chu K R. The electron cyclotron maser[J]. Reviews ofModern Physics, 2004, 76(2): 489-540.[2] Chu K R and Chen H Y, et al.. Theory and experiment ofultrahigh-gain gyrotron traveling wave amplifier[J]. IEEETransactions on Plasma Science, 1999, 27(2): 391-404.[3] Chu K R and Chen H Y, et al.. Ultrahigh gain gyrotrontraveling wave amplifier[J]. Physical Review Letters, 1998,81(21): 4760-4763.[4] Calame J P and Garven M, et al.. Gyrotron-travelingwave-tube circuit based on lossy ceramics[J]. IEEETransactions on Electron Devices, 2002, 49(8): 1469-1477.[5] 纵啸宇,薛谦忠,杜朝海. 损耗介质加载Ka波段TE01模回旋行波管放大器稳定性的分析[J]. 电子与信息学报, 2009, 31(6):1483-1486.Zong Xiao-yu, Xue Qian-zhong, and Du Chao-hai. Stabilitystudy of a Ka-band lossy dielectric-loaded TE01 modegyrotron traveling-wave-tube amplifier[J]. Journal ofElectronics Information Technology, 2009, 25(5):1483-1486.[6] Du Chao-hai, Liu Pu-kun, and Xue Qian-zhong, et al.. Effectof a backward wave on the stability of an ultrahigh gaingyrotron traveling-wave amplifier[J]. Physics of Plasmas,2008, 15(123107): 1-8.[7] Park G S, Park S Y, and Kyser R H, et al.. Broadbandoperation of a Ka-band tapered gyro-traveling waveamplifier[J]. IEEE Transactions on Plasma Science, 1994,22(5): 536-543.[8] Chong C K, McDermott D B, Luhmann, and N C Jr, et al..Large-singal operation of a third-harmonic slotted gyro-TWTamplifier[J]. IEEE Transactions on Plasma Science, 199826(3): 500-507.[9] Garven M and Calame J P, et al.. A gyrotron-traveling-wavetube amplifier experiment with a ceramic loaded interactionregion[J]. IEEE Transactions on Plasma Science, 2002, 30(3):885-893.[10] Bratman V L, Cross A W, and Denisov G G, et al.. High-gainwide-band gyrotron traveling wave amplifier with a helicallycorrugated waveguide[J]. Physical Review Letters, 2000,84(12): 2746-2749.[11] Pershing D E and Nguyen K T, et al.. A TE11 Ka-bandgyro-TWT amplifier with high-average power compatibledistributed loss[J]. IEEE Transactions on Plasma Science,2004, 32(3): 947-956.[12] Nguyen K T and Calame J P, et al.. Design of a Ka-bandgyro-TWT for radar applications[J]. IEEE Transactions onElectron Devices, 2001, 48(1): 108-115.[13] Du Chao-hai, Xue Qian-zhong, and Liu Pu-kun. Loss-inducedmodal transition in a dielectric-coated metal cylindricalwaveguide for gyro-traveling-wave-tube applications[J]. IEEEElectron Device Letters, 2008, 29(11): 1256-1258.[14] Du Chao-hai, Xue Qian-zhong, and Liu Pu-kun, et al.. Modaltransition and reduction in a lossy dielectric-coatedwaveguide for gyrotron-traveling-wave tube amplifierapplications[J]. IEEE Transactions on Electron Devices, 2009,56(5): 839-845.[15] 殷瑞剑, 刘濮鲲. 3mm回旋行波放大器单阳极磁控注入式电子枪的设计[J]. 电子与信息学报, 2008, 30(6): 1507-1510.Yin Rui-jian and Liu Pu-kun. Design of a single-anodemagnetron-injected-gun for the 3mm GYRO-TWTamplifiers[J]. Journal of Electronics InformationTechnology, 2008, 30(6): 1507-1510.
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出版历程
  • 收稿日期:  2009-06-16
  • 修回日期:  2010-02-04
  • 刊出日期:  2010-07-19

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