1984
DOI: 10.1007/bf01041396
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Coupled-resonator gyrotrons with mode conversion

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Cited by 46 publications
(9 citation statements)
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“…Such choice provides the highest coupling of the generating beam with the operating mode and a zero energy transfer of this beam to the parasitic mode TE 62 . For the absorbing beam, the coupling to the operating mode is zero while the coupling coefficients to the co-and counter-rotating modes TE 14 are equal and big enough in order to ensure that the beam withdraws energy from the spurious modes and thus suppresses the competing modes without influencing the operating mode. The estimates derived from the adiabatic theory show that the most simple scheme with a cut at the outer emitter (see Table 1) and an inner emitter with a radius of 3.7 mm (from which the generating beam originates) is not feasible because in this case, the radius of the emitter of the absorbing beam is only 1.6 mm and is located extremely close to the emitter of the generating beam.…”
Section: A Scheme With An Additional Absorbing Beammentioning
confidence: 99%
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“…Such choice provides the highest coupling of the generating beam with the operating mode and a zero energy transfer of this beam to the parasitic mode TE 62 . For the absorbing beam, the coupling to the operating mode is zero while the coupling coefficients to the co-and counter-rotating modes TE 14 are equal and big enough in order to ensure that the beam withdraws energy from the spurious modes and thus suppresses the competing modes without influencing the operating mode. The estimates derived from the adiabatic theory show that the most simple scheme with a cut at the outer emitter (see Table 1) and an inner emitter with a radius of 3.7 mm (from which the generating beam originates) is not feasible because in this case, the radius of the emitter of the absorbing beam is only 1.6 mm and is located extremely close to the emitter of the generating beam.…”
Section: A Scheme With An Additional Absorbing Beammentioning
confidence: 99%
“…In the designed EOS, the electron trajectories are far enough from the cavity wall in order to avoid an intersection of the beam by the entrance cone of the cavity in the case of a small misalignment. For the chosen radii, the most dangerous modes are TE 14 and TE 62 at the fundamental cyclotron resonance.…”
Section: A Scheme With Two Generating Beamsmentioning
confidence: 99%
“…In the studies of coupled cavities with mode conversion, quasiantisymmetric modes were mainly considered [5]. These modes in gyrotrons have a comparatively narrow range of magnetic fields and accelerating voltages, in which the starting current is less than the starting current of the quasisymmetric mode.…”
Section: Institute Of Appliedmentioning
confidence: 99%
“…High-efficiency gyrotrons with CCMC-type cavities were studied for comparatively low modes (kR ≈ 10, where k = 2π/λ is the wave number and R is the cavity radius) [5]. The efficiency of gyrotrons with echelette and CCMC cavities at high modes was fairly small [3,6,7].…”
Section: Institute Of Appliedmentioning
confidence: 99%
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