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新型高效率二次諧波寬帶可調(diào)復合互作用回旋管

劉本田

劉本田. 新型高效率二次諧波寬帶可調(diào)復合互作用回旋管[J]. 電子與信息學報, 2006, 28(4): 760-764.
引用本文: 劉本田. 新型高效率二次諧波寬帶可調(diào)復合互作用回旋管[J]. 電子與信息學報, 2006, 28(4): 760-764.
Liu Ben-tian. A New Type of Highly Efficient, Second Harmonic, Broadband Tunable Gyrotron Device Utilizing a Hybrid Interaction Scheme[J]. Journal of Electronics & Information Technology, 2006, 28(4): 760-764.
Citation: Liu Ben-tian. A New Type of Highly Efficient, Second Harmonic, Broadband Tunable Gyrotron Device Utilizing a Hybrid Interaction Scheme[J]. Journal of Electronics & Information Technology, 2006, 28(4): 760-764.

新型高效率二次諧波寬帶可調(diào)復合互作用回旋管

A New Type of Highly Efficient, Second Harmonic, Broadband Tunable Gyrotron Device Utilizing a Hybrid Interaction Scheme

  • 摘要: 該文利用回旋管注-波模式耦合理論,提出了返波振蕩-速調(diào)群聚-行波放大復合互作用回旋管工作原理。理論分析表明,Ka波段二次諧波連續(xù)磁調(diào)諧復合互作用回旋管的工作效率高達40%,磁調(diào)諧帶寬為10%。利用該復合互作用工作原理,回旋管振蕩器可實現(xiàn)毫米波電磁輻射源的高效率、高功率輸出及寬頻帶連續(xù)磁調(diào)諧。
  • Granatstein V L, Levush B, Danly B G, Parker R K. A quarter century of gyrotron research and development. IEEE Trans. Plasma Sci., 1997, 25(6): 13221334. .[2]Hirshfield J L, Wachtel J M. Electron cyclotron maser[J].Phys. Rev. Lett.1964, 12(5):533-[3]Barker R J, Schamiloglu E. High-power Microwave Sources and Technologies. New York, IEEE Press, 2001: 155196. .[4]Gantenbein G, Borie E, Dammertz G, et al.. Experimental results and numerical simulations of a high power 140 GHz gyrotron. IEEE Trans. on Plasma Sci., 1994, 22(5): 861870. .[5]Guo H, Gyrotron BWO. Symposium on Novel Methods for Generation of Electromagnetic Radiation. Yale, 1983: 1.5.[6]Park S Y, Kyser R H, Armstrong C M, et al.. Experimental study of a Ka-band gyrotron backward wave oscillator. IEEE Trans. on Plasma Sci., 1990, 18(3): 321325. .[7]Kou C S, Chen S H, Barnett L R, et al.. Experimertal study of an injection-locked gyrotron backward wave oscillator[J].Phys. Rev. Lett.1993, 70(7):924-[8]Antakov I I, Zasypkin E V, et al.. 35GHz radar gyroklystrons, Con.Digest 18th Int. Conf. on Infrared and Millimeter Waves. Colchester, UK, 1993: 338.339.[9]Chu K R, Chen H Y, Hung C L, et al.. Theory and experiment of ultra-high gain gyrotron traveling wave amplifier. IEEE Trans.on Plasma Sci., 1999, 27(2): 391404. .[10]Wang Q S, McDermott D B, Luhmann N C. Operation of a stable 200 kW, second harmonic gyro-TWT amplifier. IEEE Trans. on Plasma Sci., 1996, 24(3): 700706. .[11]Zasypkin E V, Moiseev M A, Gachev I G, et al.. Study of high-power Ka-band second-harmonic gyroklystron amplifier. IEEE Trans.on Plasma Sci., 1996, 24(3): 666670.[12]Guo H, Chen S H, Granatstein V L, et al.. Operation of a highly overmoded, harmonic-multiplying, wideband gyrotron amplifier[J].Phys. Rev. Lett.1997, 79(3):515-[13]Nusinovich G S, Dumbrajs O. Theory of gyro-BWO with tapered magnetic field and waveguide cross section[J].IEEE Trans. on Plasma Sci.1996, 24(3):620-[14]Guo H, Chen L, Keren H L, Hirshfield J. Measurements of gain for slow cyclotron waves on an annular electron beam. Phys. Rev. Lett., 1982, 49(10): 912. .[15]Gaponov A V. Relativistic dispersion equations for waveguidesystems with helical and trochoidal electron Beams. Izv. VUZov. Radiofiz,1961, 4(3): 547.560.[16]Fliflet A W. Linear and non-linear theory of the doppler-shifted cyclotron resonance maser based on TE and TM waveguide modes[J].Int. J. Electronics.1986, 61(6):1049-[17]Nusinovich G S, Li H. Theory of gyro-travelling-wave tubes at cyclotron harmonics[J].Int. J. Electronics.1992, 72(5,6):895-[18]Zhao J, Guo H, Nusinovich G S, et al.. Studies of a three-stage inverted gyrotwystron[J].IEEE Trans.on Plasma Sci.2000, 28(3):657-
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出版歷程
  • 收稿日期:  2004-09-08
  • 修回日期:  2004-12-09
  • 刊出日期:  2006-04-19

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