研究生: |
邱陳琦 Chen Chi Chiu |
---|---|
論文名稱: |
高功率寬頻磁旋行波放大器之理論研究 Theoretic Investigation of Gyrotron Traveling Wave Tube Amplifier with High Power and Broad-Band Capabilities |
指導教授: |
朱國瑞
Kwo Ray Chu |
口試委員: | |
學位類別: |
博士 Doctor |
系所名稱: |
理學院 - 物理學系 Department of Physics |
論文出版年: | 2007 |
畢業學年度: | 95 |
語文別: | 英文 |
論文頁數: | 70 |
中文關鍵詞: | 磁旋管 、磁旋行波放大器 、絕對不穩定 、飽和功率 、飽和增益 、頻寬 |
外文關鍵詞: | Gyrotron, Gyro-TWT, Absolute instability, saturated power, saturated gain, bandwidth |
相關次數: | 點閱:2 下載:0 |
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High power and broad-band gyrotron traveling wave tube amplifier (gyro-TWT) was required for advanced radar applications, remote sensing, imaging, and space object identification in 92-94 GHz atmospheric window. As is well known, the operation of gyro-TWT was largely restricted by absolute instability which is a more serious problem to gyro-TWT than to conventional TWT, since gyro-TWT usually operates near the cut off frequency of the waveguide.
Beginning from the study of various absolute instabilities in a high-order, TE01 mode, distributed-loss gyro-TWT, a systematic optimization of the performance was then proposed under the zero-drive stable condition. This device is recently designed and currently in operation at UC Davis, which can be taken as an illustration of a guide to achieve high power and broad bandwidth. The optimization processes addressed here can be applied to other gyro-TWT design as well.
The development of W-band TE01 mode gyro-TWT is collaboration between NTHU and UC Davis groups. The experimental works are conducted in the United States, while the simulation works are supported by NTHU in Taiwan. The current status on the UC Davis experiments and the corresponding simulation works are reported.
High power and broad-band gyrotron traveling wave tube amplifier (gyro-TWT) was required for advanced radar applications, remote sensing, imaging, and space object identification in 92-94 GHz atmospheric window. As is well known, the operation of gyro-TWT was largely restricted by absolute instability which is a more serious problem to gyro-TWT than to conventional TWT, since gyro-TWT usually operates near the cut off frequency of the waveguide.
Beginning from the study of various absolute instabilities in a high-order, TE01 mode, distributed-loss gyro-TWT, a systematic optimization of the performance was then proposed under the zero-drive stable condition. This device is recently designed and currently in operation at UC Davis, which can be taken as an illustration of a guide to achieve high power and broad bandwidth. The optimization processes addressed here can be applied to other gyro-TWT design as well.
The development of W-band TE01 mode gyro-TWT is collaboration between NTHU and UC Davis groups. The experimental works are conducted in the United States, while the simulation works are supported by NTHU in Taiwan. The current status on the UC Davis experiments and the corresponding simulation works are reported.
[1] K.R. Chu, Rev. Mod. Phys. 76(2), 489, 2004.
[2] P. Forman, Rev. Mod. Phys. 67, 397, 1995.
[3] W. C. Tsai, T. H. Chang, N.C. Chen, K.R. Chu, H.H. Song, and N.C. Luhmann, Jr., Phys. Rev. E, 70, 056402 (2004).
[4] K.R. Chu, H.Y. Chen, C.L. Hung, T.H. Chang, L.R. Barnett S.H. Chen, and T.T. Yang, Phys. Rev. Lett. 81, 4760 (1998).
[5] K. T. Nguyen, J. P. Calame, D. E. Pershing, B. G. Danly, M. Garven, B. Levush, and T. M. Antonsen, IEEE Trans. Plasma Sci. 48, 108 (2001).
[6] H. H. Song, D. B. McDermott, Y. Hirata, L. R. Barnett, C. W. Domier, H. L. Hsu, T. H. Chang, W. C. Tsai, K. R. Chu, and N. C. Luhmann, Jr., Phys. Plasmas 11, 2935 (2004).
[7] M. Garven, J. P. Calame, B. G. Danly, K. T. Nguyen, B. Levush, F. N. Wood, and D. E. Pershing, IEEE Trans. Plasma Sci. 30, 885 (2002)
[8] C. K. Chong, D. B. McDermott, and N. C. Luhmann, Jr., IEEE Trans. Plasma Sci. 26, 500 (1998).
[9] Q. S. Wang, D. B. McDermott, and N. C. Luhmann, Jr., Phys. Rev. Lett. 75, 4322 (1995).
[10] K. R. Chu, H. Guo, and V. L. Granatstein, Phys. Rev. Lett. 78, 4661 (1997).
[11] H. Guo, S. H. Chen, V. L. Granatstein, J. Rogers, G. S. Nusinovich, M. Waters, B. Levush, and W. J. Chen, Phys. Rev. Lett. 79, 515 (1997).
[12] J. Rodgers, H. Guo, G. S. Nusinovich, and V. L. Granatstein, IEEE Trans. Electron Devices 48, 2434 (2001).
[13] V. L. Bratman, A. W. Gross, G. G. Denisov, W. He, A. D. R. Phelps, K. Ronald, S. V. Samsonov, C. G. Whyte, and A. R. Young, Phys. Rev. Lett., vol. 84, pp. 2746–2749, (2000).
[14] K. R. Chu, IEEE Trans. Plasma Sci. 30, 903 (2002).
[15] L. A. Hoffman, K. H. Hurlbut, D. E. Kind, and H. J. Wintroub, IEEE Trans. Microwave Theory Tech., vol. MTT-17, pp. 1145–1149, (1969).
[16] D. B. McDermott, H. H. Song, Y. Hirata et al., IEEE Trans. Plasma Sci. 30, 894 (2002).
[17] V. L. Granatstein, B. Levush, B. G. Danly, and R. K. Parker, IEEE Trans. Plasma Sci. 25, 1322 (1997).
[18] M. Blank, B. G. Danly, B. Levush et al., Phys. Plasmas 6, 4405 (1999).
[19] M. Blank, K. Felch, B. G. James et al., IEEE Trans. Plasma Sci. 30, 865 (2002).
[20] K. R. Chu, and Anthony T. Lin, IEEE Trans. Plasma Sci. 16, 90 (1988).
[21] G.. DOHLER, Int. J. Electron. 56, 617–627 (1984).
[22] G.. DOHLER, Int. J. Electron. 56, 629–640 (1984).
[23] C. S. Kou and Fouries Tseng, Phys. Plasmas 5 2454 (1998).