2012
DOI: 10.1143/jjap.51.126601
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Calculations of Starting Currents and Frequencies in Frequency-Tunable Gyrotrons

Abstract: Cold cavity and self-consistent formalisms for starting current and frequency calculations in frequency-tunable gyrotrons are summarized. Numerical solution schemes of the corresponding equations are discussed. A specific case is analyzed in detail.

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Cited by 17 publications
(5 citation statements)
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“…To investigate the physical processes underlying these results, the dependences of the oscillation power and the frequency on several parameters were calculated using a self-consistent code, 8 in which the output power P from the cavity exit and the wave frequency f are calculated by simultaneously solving for both the electron motion and the electric field growth in the cavity. 8 The input parameters for this code are V k , I c , B, the radius of the annular electron beam at the cavity R b , and the pitch factor of the electrons a.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…To investigate the physical processes underlying these results, the dependences of the oscillation power and the frequency on several parameters were calculated using a self-consistent code, 8 in which the output power P from the cavity exit and the wave frequency f are calculated by simultaneously solving for both the electron motion and the electric field growth in the cavity. 8 The input parameters for this code are V k , I c , B, the radius of the annular electron beam at the cavity R b , and the pitch factor of the electrons a.…”
Section: Discussionmentioning
confidence: 99%
“…8 The input parameters for this code are V k , I c , B, the radius of the annular electron beam at the cavity R b , and the pitch factor of the electrons a. The values of R b and a were determined from electron trajectories that were calculated using the EGUN code.…”
Section: Discussionmentioning
confidence: 99%
“…And in Figure 3, we can see that the major competing modes, TE 24,10 and TE 26,10 for TE 25,10 , are fairly well separated. Considering the higher longitudinal index modes, ones can ignore the modes of TE 25,10,2 and TE 25,10,3 , because they have much lower quality factors than the modes whose value of q is 1 (i.e., the TE 25,10,1 mode in the present case) [15,16]. Hence, the TE 25,10 mode was chosen as the operating mode for the…”
Section: Mode Selectionmentioning
confidence: 99%
“…Starting current estimation can be done in a classic way [4,10], but it can also be found by iterating the time simulation for different beam current values until stable power at the output and a stable RF field can be observed. This is quite a convenient method as it does not need extra programming, but it does require computation time.…”
Section: Starting Current Estimation In Time Dependent Theoremmentioning
confidence: 99%