TY - JOUR
T1 - Frequency-Replaceable Ferroelectric Cathode Gyrotron for the Entire Ka-Band Using Replaceable Resonator
AU - Avraham, Eviatar
AU - Ben-Moshe, Roey
AU - Pilossof, Moritz
AU - Einat, Moshe
N1 - Publisher Copyright:
© 2016 IEEE.
PY - 2016/5
Y1 - 2016/5
N2 - A modular, mid-power, Ka-band frequency (27-40 GHz) gyrotron is reported. The gyrotron is known as a dominant tube for millimeter waves, but once fabricated its frequency changing is limited. In this paper, a gyrotron with a replaceable resonator was designed and built. By a rather simple action of resonator replacement, the operating frequency of the gyrotron can be replaced. The use of a ferroelectric cathode supports a quick opening and closing of the tube for the resonator replacement in less than half an hour. With the view of covering a wide range of frequencies, a wide range magnetic field pulsed copper solenoid was designed, supporting the gyrotron operation on either the fundamental or the second harmonic of the electron-cyclotron frequency. The gyrotron design is based on a ferroelectric electron gun designed and built to provide the appropriate electron beam to a wide variety of resonators, operating at the fundamental or at the second harmonic. The gyrotron with two differently designed resonators has been constructed and tested in the TE01, TE21, and TE11 modes at 39, 31, and 27 GHz, respectively. With an accelerating beam voltage of-35 kV and a beam current of ∼ 1-1.7 A, an output power of ∼ 1-6 kW was obtained at single pulse and at ∼ 200-ns micropulse in ∼ 6-μs macropulse with ∼ 25 % duty cycle. In addition, the system was operated with 5-s repetition rate for half an hour, and a high stability was measured for all the mentioned frequencies.
AB - A modular, mid-power, Ka-band frequency (27-40 GHz) gyrotron is reported. The gyrotron is known as a dominant tube for millimeter waves, but once fabricated its frequency changing is limited. In this paper, a gyrotron with a replaceable resonator was designed and built. By a rather simple action of resonator replacement, the operating frequency of the gyrotron can be replaced. The use of a ferroelectric cathode supports a quick opening and closing of the tube for the resonator replacement in less than half an hour. With the view of covering a wide range of frequencies, a wide range magnetic field pulsed copper solenoid was designed, supporting the gyrotron operation on either the fundamental or the second harmonic of the electron-cyclotron frequency. The gyrotron design is based on a ferroelectric electron gun designed and built to provide the appropriate electron beam to a wide variety of resonators, operating at the fundamental or at the second harmonic. The gyrotron with two differently designed resonators has been constructed and tested in the TE01, TE21, and TE11 modes at 39, 31, and 27 GHz, respectively. With an accelerating beam voltage of-35 kV and a beam current of ∼ 1-1.7 A, an output power of ∼ 1-6 kW was obtained at single pulse and at ∼ 200-ns micropulse in ∼ 6-μs macropulse with ∼ 25 % duty cycle. In addition, the system was operated with 5-s repetition rate for half an hour, and a high stability was measured for all the mentioned frequencies.
KW - Ferroelectric cathode
KW - Ka-band
KW - ferroelectric electron gun
KW - tunable gyrotron.
UR - http://www.scopus.com/inward/record.url?scp=84977950718&partnerID=8YFLogxK
U2 - 10.1109/TED.2016.2536758
DO - 10.1109/TED.2016.2536758
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AN - SCOPUS:84977950718
SN - 0018-9383
VL - 63
SP - 2097
EP - 2103
JO - IEEE Transactions on Electron Devices
JF - IEEE Transactions on Electron Devices
IS - 5
M1 - 7433440
ER -