Influence of the energy and velocity spread in the electron beam on the starting conditions and efficiency of a gyrotron
暂无分享,去创建一个
[1] V. Zapevalov,et al. Influence of Aftercavity Interaction on Gyrotron Efficiency , 2004 .
[2] V. K. Lygin,et al. Numerical Simulation Models of Forming Systems of Intense Gyrotron Helical Electron Beams , 2001 .
[3] V. Zapevalov,et al. Efficiency Enhancement of the Relativistic Gyrotron , 2001 .
[4] L. G. Popov,et al. Development of 170 GHz/1 MW Russian gyrotron for ITER , 2001 .
[5] B. Piosczyk,et al. On the negative-mass instability in gyrotrons , 2000, 25th International Conference on Infrared and Millimeter Waves (Cat. No.00EX442).
[6] O. Dumbrajs,et al. Generalized gyrotron theory with inclusion of electron velocity and energy spreads , 1999 .
[7] M. Glyavin,et al. Experimental studies of gyrotron electron beam systems , 1999 .
[8] Mikhail A. Moiseev,et al. Development of 1 mw output power level gyrotron for ITER , 1998 .
[9] V. K. Lygin,et al. Numerical simulation of intense helical electron beams with the calculation of the velocity distribution functions , 1995 .
[10] G. P. Saraph,et al. Multifrequency theory of high power gyrotron oscillators , 1992 .
[11] Gregory S. Nusinovich,et al. Relativistic gyrotrons and cyclotron autoresonance masers , 1981 .
[12] E. Sokolov,et al. Starting conditions of a CRM monotron in the presence of scatter of the velocities of the electrons , 1977 .
[13] M. I. Petelin,et al. The induced radiation of excited classical oscillators and its use in high-frequency electronics , 1967 .