1970
DOI: 10.1109/t-ed.1970.17123
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Starting conditions for backward-wave oscillators with large loss and large space charge

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Cited by 17 publications
(12 citation statements)
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“…The Pierce type small-signal analysis of a TWT [1][2][3][4][5][6][7][8], when interpreted for the propagation of energy in the backward direction, usually gives the start-oscillation condition of the device in terms of the Pierce's normalized circuit-gain CN, and the Pierce's normalized space-charge parameter QC [1][2][3][4][5][6]. Under no-loss assumption, the critical circuit-gain follows a co-sinusoidal nature [3,7,20], given as:…”
Section: Discussionmentioning
confidence: 99%
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“…The Pierce type small-signal analysis of a TWT [1][2][3][4][5][6][7][8], when interpreted for the propagation of energy in the backward direction, usually gives the start-oscillation condition of the device in terms of the Pierce's normalized circuit-gain CN, and the Pierce's normalized space-charge parameter QC [1][2][3][4][5][6]. Under no-loss assumption, the critical circuit-gain follows a co-sinusoidal nature [3,7,20], given as:…”
Section: Discussionmentioning
confidence: 99%
“…The phenomenon of backward-wave oscillation, at or near the upper band-edge of a helix slow-wave structure (SWS) of a traveling-wave tube (TWT) [1][2][3][4][5][6][7][8], is one of the limiting factors for multi-octave operation of the device. Over the past decade, the need for development of compact multi-octave micro-TWTs has rekindled the interest in studying this phenomenon [9][10][11][12][13][14][15][16][17][18][19][20].…”
Section: Introductionmentioning
confidence: 99%
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“…The gain parameter of a linear lossy TWT that corresponds to the start-oscillation condition can be expressed by Equation (1) [6]. For gyro-TWT, the gain parameter is described as Equation (2) [7].…”
Section: Conversion Of Linear Twt Parameters To Gyro-twtmentioning
confidence: 99%