Abstract

The self-excitation of asymmetric modes is one of the main factors limiting the long-pulse operation of the relativistic triaxial klystron amplifier (TKA). Research studies have revealed that the asymmetric TM modes with negative beam loading conductance (Ge/G0) in the bunching cavities are the main culprits of self-excitation. The existing studies focus on passively destroying the growth of asymmetric TM modes, but we attempt to actively suppress their self-excitation in this paper. Investigation results demonstrate that the employment of single-gap bunching cavities can significantly reduce the risk of self-excitation of asymmetric TM modes, as the Ge/G0 of asymmetric TMn11 modes in single period structures are positive. The current modulation capacity of a single-gap bunching cavity, however, is not sufficient, so a cascade structure consisting of two groups of bunching cavities is employed to compensate for this deficiency. Based on the above conclusions, an X-band TKA device with four single-gap beam–wave interaction cavities is proposed and investigated in this paper. The three-dimensional particle-in-cell simulation results demonstrate that there is no self-excitation of asymmetric modes in the proposed X-band TKA device.

Highlights

  • The relativistic triaxial klystron amplifier (TKA), with its advantages of frequency-locking and phase-locking,1,2 is one of the most promising high power microwave (HPM) sources for power combination

  • According to the theory of TKA devices, the drift tube can only cut off the operation mode: TM01 mode

  • The evolution of asymmetric modes will lead to output pulse shortening, and even worse, completely destroy the operation of TKA devices

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Summary

INTRODUCTION

The relativistic triaxial klystron amplifier (TKA), with its advantages of frequency-locking and phase-locking, is one of the most promising high power microwave (HPM) sources for power combination. To achieve active suppression of the self-excitation of asymmetric modes, the mechanism of mode competition in the initial structure is further investigated, and an improved structure with four single-gap beam–wave interaction cavities is proposed in this paper. When single-gap beam–wave interaction cavities are adopted, the risk for self-excitation of asymmetric TMn11 modes is significantly reduced, and this will be further discussed in the main part of this paper. This paper is organized as follows: in Sec. II, the self-excitation of asymmetric modes observed in the initial X-band TKA device is described.

DESCRIPTION OF MODE COMPETITION AND PASSIVE SUPPRESSION METHODS
MECHANISM OF ACTIVE SUPPRESSION METHODS
Suppression mechanism of single-gap bunching cavities
Compensation for the insufficient modulation of single-gap bunching cavities
VERIFICATION BY 3D PIC SIMULATION
Findings
CONCLUSIONS
Full Text
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