A study of sub-THz gyrotron devices with external injection signals

碩士 === 南臺科技大學 === 光電工程系 === 105 === The gyrotron traveling-wave amplifiers(gyro-TWAs) is a high power,broadband,millimeter-wave amplifier,applied in communication,military radarNMR(nuclear magnetic resonance). This study presents a comparative three schemes analysis of fourth-harmonic multiplying gy...

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Main Author: 高文哲
Other Authors: Yi Sheng Yeh
Format: Others
Language:zh-TW
Published: 2017
Online Access:http://ndltd.ncl.edu.tw/handle/48473400496788347372
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spelling ndltd-TW-105STUT01240102017-08-06T04:23:57Z http://ndltd.ncl.edu.tw/handle/48473400496788347372 A study of sub-THz gyrotron devices with external injection signals 注入功率驅動次太赫茲磁旋管研究 高文哲 碩士 南臺科技大學 光電工程系 105 The gyrotron traveling-wave amplifiers(gyro-TWAs) is a high power,broadband,millimeter-wave amplifier,applied in communication,military radarNMR(nuclear magnetic resonance). This study presents a comparative three schemes analysis of fourth-harmonic multiplying gyro-TWA, M=1, M=2 and M=4, respectively. Absolute instabilities in the gyro-TWA are suppressed by distributed-wall losses and a mode selective circuit. The amplification of the waves in a gyro-TWA depends on the lengths of the sections, and the simulated results show that the gain increases for all schemes, as the length of the lossy section or the length of the copper section increases. Finally, at a different multiplier ratio (M = 1, M = 2, M = 4) there is almost the same saturated output powers 15kW and saturated gain 48dB. The fourth chapter is the 900 GHz injection signals drives gyrotron, in order to suppress the mode to avoid competition with the mode,first to use the injection TE89 mode backward power to drive the oscillator to form a phase-locked; and to change the power from the forward injection mode , To the cluster the electron beam amplification mode of operation, suppress the mode, but the results show no matter how much power is injected. Therefore, it is shown that there are two kinds of steady-state solutions, which can not completely suppress the competition mode of the fundamental harmonics, by the backward of and forward wave to the oscillator. In order to avoid the competition of the oscillator mode, this study will reduce the applied magnetic field B0, change the length L5, input segment L1, isolation length L3 and current Ib. From these results, the optimal operating parameters are L1=1.09cm,L2=0.3cm,L3=0.4cm,L4=0.3cm,L5=1.1cm,B0=166.8kG,Vb=30kV,Ib=3A,α=1.1, =5%。Based on the relationship between the output power of the Gyro-TWT and the input power , the results show that the linear gain is about 45dB between Pin = 10-4 ~ 0.05W and Pin = 0.1W saturation gain of 50dB. In addition, the Gyro-TWT saturation power Psat and frequency f relationship shown, the operating frequency of 888.7GHz, maximum power of 6.2kW, bandwidth is about 0.6GHz,gain of 47dB. Yi Sheng Yeh 葉義生 2017 學位論文 ; thesis 53 zh-TW
collection NDLTD
language zh-TW
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sources NDLTD
description 碩士 === 南臺科技大學 === 光電工程系 === 105 === The gyrotron traveling-wave amplifiers(gyro-TWAs) is a high power,broadband,millimeter-wave amplifier,applied in communication,military radarNMR(nuclear magnetic resonance). This study presents a comparative three schemes analysis of fourth-harmonic multiplying gyro-TWA, M=1, M=2 and M=4, respectively. Absolute instabilities in the gyro-TWA are suppressed by distributed-wall losses and a mode selective circuit. The amplification of the waves in a gyro-TWA depends on the lengths of the sections, and the simulated results show that the gain increases for all schemes, as the length of the lossy section or the length of the copper section increases. Finally, at a different multiplier ratio (M = 1, M = 2, M = 4) there is almost the same saturated output powers 15kW and saturated gain 48dB. The fourth chapter is the 900 GHz injection signals drives gyrotron, in order to suppress the mode to avoid competition with the mode,first to use the injection TE89 mode backward power to drive the oscillator to form a phase-locked; and to change the power from the forward injection mode , To the cluster the electron beam amplification mode of operation, suppress the mode, but the results show no matter how much power is injected. Therefore, it is shown that there are two kinds of steady-state solutions, which can not completely suppress the competition mode of the fundamental harmonics, by the backward of and forward wave to the oscillator. In order to avoid the competition of the oscillator mode, this study will reduce the applied magnetic field B0, change the length L5, input segment L1, isolation length L3 and current Ib. From these results, the optimal operating parameters are L1=1.09cm,L2=0.3cm,L3=0.4cm,L4=0.3cm,L5=1.1cm,B0=166.8kG,Vb=30kV,Ib=3A,α=1.1, =5%。Based on the relationship between the output power of the Gyro-TWT and the input power , the results show that the linear gain is about 45dB between Pin = 10-4 ~ 0.05W and Pin = 0.1W saturation gain of 50dB. In addition, the Gyro-TWT saturation power Psat and frequency f relationship shown, the operating frequency of 888.7GHz, maximum power of 6.2kW, bandwidth is about 0.6GHz,gain of 47dB.
author2 Yi Sheng Yeh
author_facet Yi Sheng Yeh
高文哲
author 高文哲
spellingShingle 高文哲
A study of sub-THz gyrotron devices with external injection signals
author_sort 高文哲
title A study of sub-THz gyrotron devices with external injection signals
title_short A study of sub-THz gyrotron devices with external injection signals
title_full A study of sub-THz gyrotron devices with external injection signals
title_fullStr A study of sub-THz gyrotron devices with external injection signals
title_full_unstemmed A study of sub-THz gyrotron devices with external injection signals
title_sort study of sub-thz gyrotron devices with external injection signals
publishDate 2017
url http://ndltd.ncl.edu.tw/handle/48473400496788347372
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