An Experimental Study of the Influence of the Longitudinal Magnetic-Field Distribution Profile on the Output Characteristics of a Gyrotron

[1]  Gaofeng Liu,et al.  Effects of Different Magnetic Field Profiles on Output Power and Efficiency of a Second-Harmonic Gyrotron , 2019, IEEE Transactions on Plasma Science.

[2]  O. Dumbrajs,et al.  Efficiency of gyrotrons with a tapered magnetic field in the regime of soft self-excitation , 2018 .

[3]  John Jelonnek,et al.  Magnetic field profile analysis for gyrotron experimental investigation , 2017 .

[4]  John Jelonnek,et al.  A comparative study on the modeling of dynamic after-cavity interaction in gyrotrons , 2015 .

[5]  M. Glyavin,et al.  The K(a)-band 10-kW continuous wave gyrotron with wide-band fast frequency sweep. , 2012, The Review of scientific instruments.

[6]  T. Idehara,et al.  Application of Continuously Frequency-Tunable 0.4 THz Gyrotron to Dynamic Nuclear Polarization for 600 MHz Solid-State NMR , 2012 .

[7]  Stefan Illy,et al.  2.2-MW Record Power of the 170-GHz European Preprototype Coaxial-Cavity Gyrotron for ITER , 2010, IEEE Transactions on Plasma Science.

[8]  G. Nusinovich,et al.  Analysis of aftercavity interaction in gyrotrons , 2009 .

[9]  Toshitaka Idehara,et al.  Development of high‐harmonic gyrotrons using a permanent magnet system , 2004 .

[10]  V. Zapevalov,et al.  Influence of Aftercavity Interaction on Gyrotron Efficiency , 2004 .

[11]  Yu. Bykov,et al.  24-84-GHz gyrotron systems for technological microwave applications , 2003, IEEE Transactions on Plasma Science.

[12]  G. Gantenbein,et al.  Gyrotron with a tapered external magnetic field , 1990 .

[13]  G. Nusinovich.  Linear theory of a gyrotron with weakly tapered external magnetic field , 1988 .

[14]  A. P. Keier.  Electron flux bunching with spread in electron velocities in a gyroklystron with a nonuniform magnetic field , 1978 .