PIC Simulations of Ka-band Ultra-Short Pulse Oscillator with Resonance Cyclotron Absorber in the Feedback Loop
PIC Simulations of Ka-band Ultra-Short Pulse Oscillator with Resonance Cyclotron Absorber in the Feedback Loop
复制标题
反馈环路中带有谐振回旋吸收器的Ka波段超短脉冲振荡器的PIC仿真
DOI:
10.1051/epjconf/201818701021
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发表时间:
2018
期刊:
影响因子:
--
通讯作者:
Jelonnek
中科院分区:
文献类型:
--
作者:
Ginzburg;Denisov;Vilkov;Zotova;Sergeev;Samsonov;Jelonnek
In [1, 2] it was shown that periodical trains of ultrashort microwave pulses (USP) can be produced in a two-section microwave oscillator consisting of an amplifier and a nonlinear (saturable) absorber in the feedback loop. In such a system, the process of pulse formation is based on the effect of passive modelocking which is well known in laser physics [3]. At the present moment, the Ka-band USP oscillator with a broadband helical-waveguide gyro-TWT [4] as an active unit is under development at the Institute of Applied Physics. The saturable absorber will be realized in an auxiliary section based on the cyclotron resonance interaction with an initially rectilinear magnetized electron beam. In this case the nonlinearity of absorption is provided due to relativistic dependence of a gyrofrequency on the electrons energy. The basic parameters of the USP oscillator have been defined on the basis of a simple averaged model. This paper is devoted to the full-scale particle-in-cell (PIC) simulations of such a system based on the software CST Studio Suite [5] aimed to optimize the parameters taking into account the real conditions of the planning experiment.For simulations the computer model has been developed, in which the helical-waveguide amplifier and the cyclotron absorber were installed opposite each other (see Fig. 1). The gyro-TWT operates at the second cyclotron harmonic while the fundamental cyclotron resonance is used in the absorber unit. From the cathode ends both sections were bounded by resonance reflectors. The independent electron beams with the given parameters were entered the calculated space from the left and right ends of the corresponding sections and, after interaction, deflected in a strong transverse magnetic field to the waveguide wall. Between the oscillator sections there was a polarization-selective waveguide coupler which allows simulating the branching of the useful power to the load. Thus, the initial microwave pulse could be fed to
影响因子:
2.2
作者:
Ginzburg;Denisov;Vilkov;Sergeev;Zotova;Samsonov;Mishakin
通讯作者:
Mishakin
DOI:
--
发表时间:
2016
期刊:
影响因子:
--
作者:
N. Ginzburg;G. Denisov;M. Vilkov;I. Zotova;A. Sergeev
通讯作者:
A. Sergeev