22nd European Microwave Conference, 1992 1992
DOI: 10.1109/euma.1992.335771
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The Clinotron

Abstract: I actua device-"s o .I f aillme4e 1 6d subLrimili . ' mete wave banids i preSented.Th e clntoM e ore o eletrMagneti oscillations with increasect~~~~~~~~~~~~L LbGrQr andx~T efciecyinmLlietuer and microwavedevies with diswr fild-letrniner-io. h sumifferenc between . bakwr wbe osiltr (BWO) an clntrn 4 A~~~~~C V 4.1,I Mc0fl5l v u l eiD vdppiicaIiOwiith d 0J i uuLr k' e cl`ttir" n OCafle li-Y-wth er' !" K --H e lowrt feruvee e,t n n srrkTherauL-ng e tag an he fou0rg~agm fi^1 reld; arm vi ig,o " izu of'an it bra bea… Show more

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Cited by 37 publications
(6 citation statements)
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“…Thus there is a strong dependence of the starting current on the tilt angle, which is well-known from the experimental results [1]. Such dependence was also predicted in [5].…”
Section: The Spectrum Shape Function Issupporting
confidence: 79%
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“…Thus there is a strong dependence of the starting current on the tilt angle, which is well-known from the experimental results [1]. Such dependence was also predicted in [5].…”
Section: The Spectrum Shape Function Issupporting
confidence: 79%
“…Taking into account that in our case and , we find that the maximum beam current density is Assuming, for example, that the beam accelerating voltage is 3 kV, GHz, and , we have A/cm . This value is by several times larger compared to that used in practical clinotrons [1]. It should be noted that the maximum beam current density rapidly grows with an increase of both the operating frequency and the tilt angle.…”
Section: Steady-state Oscillationsmentioning
confidence: 80%
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