Cherenkov radiation from a pseudospark-sourced electron beam

被引:0
作者
Phelps, ADR [1 ]
Yin, H [1 ]
Cross, AW [1 ]
He, W [1 ]
Ronald, K [1 ]
机构
[1] Univ Strathclyde, Dept Phys, Glasgow G4 0NG, Lanark, Scotland
来源
HIGH ENERGY DENSITY AND HIGH POWER RF | 2003年 / 691卷
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中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Electron beam generation from a multi-gap pseudospark discharge was investigated. A pseudospark-sourced electron beam has two phases, an initial hollow cathode phase (HCP) beam followed by a conductive phase (CP) beam, The beam brightness was measured by a field-free collimator to be 10(9) and 10(11) Am(-2)rad(-2) for the hollow cathode phase (HCP) beam and the conductive phase (CP) beam respectively. The initial HCP beam from an eight-gap pseudospark discharge was applied in a Cherenkov interaction between the electron beam and the TM01 mode of a 60-cm long alumina-lined waveguide. It was found experimentally that significant microwave radiation was generated only when the dielectric was present in the interaction space. If there was no dielectric in the cylindrical waveguide, then a very small background microwave output was detected even when the guide B-field was absent. This demonstrated, in conjunction with the observation that the microwave output signal was independent of the guide magnetic field over the range 0.13 to 0.26 T, that the radiation from the experiment was due to the Cherenkov interaction mechanism. In addition, two components of the microwave pulse were observed corresponding to the two energy components of the electron beam during the pseudospark discharge breakdown. These results demonstrated that the microwave radiation was generated by Cherenkov amplification of the broadband emission from the pseudospark discharge itself A background signal level of around 100 W was measured in the frequency range 20 - 50 GHz with a percentage of (2.7 +/- 0.6)% in the frequency range 25.5 - 28.6 GHz, when the dielectric lining was removed from the maser. The frequency of the microwave output after the Cherenkov maser interaction was measured to be mainly around 25.5 GHz and the dominating mode was identified as being TM01. The duration of the microwave pulse was approximately 80 ns, with a peak power of around 2 +/- 0.2 M The gain of this amplifier was measured as 29 +/- 3 dB.
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页码:401 / 405
页数:5
相关论文
共 12 条
[1]   PRODUCTION OF HIGH-CURRENT PARTICLE BEAMS BY LOW-PRESSURE SPARK DISCHARGES [J].
CHRISTIANSEN, J ;
SCHULTHEISS, C .
ZEITSCHRIFT FUR PHYSIK A-HADRONS AND NUCLEI, 1979, 290 (01) :35-41
[2]   THE FUNDAMENTALS OF THE PSEUDOSPARK AND ITS APPLICATIONS [J].
FRANK, K ;
CHRISTIANSEN, J .
IEEE TRANSACTIONS ON PLASMA SCIENCE, 1989, 17 (05) :748-753
[3]   NONLINEAR-ANALYSIS OF HIGH-POWER CHERENKOV MASERS [J].
FREUND, HP .
PHYSICAL REVIEW LETTERS, 1990, 65 (24) :2993-2996
[4]   CERENKOV MASER OPERATION AT LOWER-MM WAVELENGTHS [J].
GARATE, E ;
COOK, R ;
HEIM, P ;
LAYMAN, R ;
WALSH, J .
JOURNAL OF APPLIED PHYSICS, 1985, 58 (02) :627-632
[5]  
GUNDERSEN MA, 1990, NATO ASI SER B
[6]   EMISSION OF MICROWAVE AND MILLIMETER WAVELENGTH RADIATION DURING HOLLOW-CATHODE DISCHARGE OPERATION OF THE BACK LIGHTED THYRATRON [J].
LIOU, R ;
FIGUEROA, H ;
MCCURDY, AH ;
KIRKMANAMEMIYA, G ;
TEMKIN, RJ ;
FETTERMAN, H ;
GUNDERSEN, MA .
APPLIED PHYSICS LETTERS, 1992, 61 (23) :2779-2881
[7]   HIGH-GAIN X-BAND DIELECTRIC CHERENKOV MASER [J].
PETER, W ;
GARATE, E ;
MAIN, W ;
FISHER, A .
PHYSICAL REVIEW LETTERS, 1990, 65 (24) :2989-2992
[8]   Microwave generation in a high voltage triggered pseudospark discharge experiment [J].
Ramaswamy, K ;
Destler, WW ;
Rodgers, J .
JOURNAL OF APPLIED PHYSICS, 1998, 83 (07) :3514-3520
[9]  
Yin H., 1999, Physical Review Special Topics-Accelerators and Beams, V2, DOI 10.1103/PhysRevSTAB.2.020701
[10]   Pseudospark-based electron beam and Cherenkov maser experiments [J].
Yin, H ;
Robb, GRM ;
He, W ;
Phelps, ADR ;
Cross, AW ;
Ronald, K .
PHYSICS OF PLASMAS, 2000, 7 (12) :5195-5205