Matches in SemOpenAlex for { <https://semopenalex.org/work/W2282383970> ?p ?o ?g. }
- W2282383970 abstract "Theoretical studies of the operation of crossed-field electron vacuum devices such as magnetrons and crossed-field amplifiers CFA have usually centered on their initial growth, taking this as an indication of their operating modes. In such an analysis one solves the equations for the density profile, the operating frequency, the growth rate, and other features of these devices. What one really obtains then are only the conditions for the device to turn on. The dominant interaction in this stage is a Rayleigh-type instability which initiates a quasilinear diffusion process whereby the electron density profile redistributes itself into a profile which will be in equilibrium with the ponderomotive-like forces produced by the growing rf fields. Eventually the rf fields will saturate and an operating device will settle into a stationary operating regime. This stage of a device’s operation is called the “saturation stage.” This latter stage involves a different set of physical interactions from the initiation stage. No longer is there a growth rate; rather the rf amplitudes have saturated and as a result, the ponderomotive-like forces have also vanished along with the quasilinear diffusion. In this saturation stage, we find that new rf modes appear. In fact, there are a total of five rf modes, two of which are the usual slow modes of the initiation stage, and three of which have fast oscillations in the vertical direction. One fast mode corresponds to a drift plasma oscillation while the other two fast modes are drift cyclotron modes. In this paper, we will describe how the drift plasma oscillation interacts and couples with the slow rf modes at the diocotron resonance. © 2006 American Institute of Physics. DOI: 10.1063/1.2199227" @default.
- W2282383970 created "2016-06-24" @default.
- W2282383970 creator A5085068263 @default.
- W2282383970 date "2005-10-25" @default.
- W2282383970 modified "2023-09-22" @default.
- W2282383970 title "Drift Resonance in High Density Nonneutral Plasmas" @default.
- W2282383970 cites W1657347807 @default.
- W2282383970 cites W1968134399 @default.
- W2282383970 cites W1968194495 @default.
- W2282383970 cites W1970946779 @default.
- W2282383970 cites W1984276925 @default.
- W2282383970 cites W1987737162 @default.
- W2282383970 cites W1995549870 @default.
- W2282383970 cites W1996952829 @default.
- W2282383970 cites W2001281912 @default.
- W2282383970 cites W2002225129 @default.
- W2282383970 cites W2018541431 @default.
- W2282383970 cites W2022262842 @default.
- W2282383970 cites W2037721994 @default.
- W2282383970 cites W2045629957 @default.
- W2282383970 cites W2060528673 @default.
- W2282383970 cites W2073234936 @default.
- W2282383970 cites W2073308339 @default.
- W2282383970 cites W2078914627 @default.
- W2282383970 cites W2091424390 @default.
- W2282383970 cites W2091920911 @default.
- W2282383970 cites W2097131835 @default.
- W2282383970 cites W2120062331 @default.
- W2282383970 cites W2149004014 @default.
- W2282383970 cites W2160408050 @default.
- W2282383970 cites W2166122888 @default.
- W2282383970 cites W2170844090 @default.
- W2282383970 cites W2400960883 @default.
- W2282383970 cites W2208364055 @default.
- W2282383970 hasPublicationYear "2005" @default.
- W2282383970 type Work @default.
- W2282383970 sameAs 2282383970 @default.
- W2282383970 citedByCount "0" @default.
- W2282383970 crossrefType "journal-article" @default.
- W2282383970 hasAuthorship W2282383970A5085068263 @default.
- W2282383970 hasConcept C114614502 @default.
- W2282383970 hasConcept C120665830 @default.
- W2282383970 hasConcept C121332964 @default.
- W2282383970 hasConcept C147120987 @default.
- W2282383970 hasConcept C180205008 @default.
- W2282383970 hasConcept C184779094 @default.
- W2282383970 hasConcept C185592680 @default.
- W2282383970 hasConcept C194257627 @default.
- W2282383970 hasConcept C207821765 @default.
- W2282383970 hasConcept C2778175000 @default.
- W2282383970 hasConcept C2778439541 @default.
- W2282383970 hasConcept C30475298 @default.
- W2282383970 hasConcept C33923547 @default.
- W2282383970 hasConcept C39527238 @default.
- W2282383970 hasConcept C46362747 @default.
- W2282383970 hasConcept C49040817 @default.
- W2282383970 hasConcept C55493867 @default.
- W2282383970 hasConcept C57879066 @default.
- W2282383970 hasConcept C62520636 @default.
- W2282383970 hasConcept C69357855 @default.
- W2282383970 hasConcept C82706917 @default.
- W2282383970 hasConcept C9930424 @default.
- W2282383970 hasConceptScore W2282383970C114614502 @default.
- W2282383970 hasConceptScore W2282383970C120665830 @default.
- W2282383970 hasConceptScore W2282383970C121332964 @default.
- W2282383970 hasConceptScore W2282383970C147120987 @default.
- W2282383970 hasConceptScore W2282383970C180205008 @default.
- W2282383970 hasConceptScore W2282383970C184779094 @default.
- W2282383970 hasConceptScore W2282383970C185592680 @default.
- W2282383970 hasConceptScore W2282383970C194257627 @default.
- W2282383970 hasConceptScore W2282383970C207821765 @default.
- W2282383970 hasConceptScore W2282383970C2778175000 @default.
- W2282383970 hasConceptScore W2282383970C2778439541 @default.
- W2282383970 hasConceptScore W2282383970C30475298 @default.
- W2282383970 hasConceptScore W2282383970C33923547 @default.
- W2282383970 hasConceptScore W2282383970C39527238 @default.
- W2282383970 hasConceptScore W2282383970C46362747 @default.
- W2282383970 hasConceptScore W2282383970C49040817 @default.
- W2282383970 hasConceptScore W2282383970C55493867 @default.
- W2282383970 hasConceptScore W2282383970C57879066 @default.
- W2282383970 hasConceptScore W2282383970C62520636 @default.
- W2282383970 hasConceptScore W2282383970C69357855 @default.
- W2282383970 hasConceptScore W2282383970C82706917 @default.
- W2282383970 hasConceptScore W2282383970C9930424 @default.
- W2282383970 hasLocation W22823839701 @default.
- W2282383970 hasOpenAccess W2282383970 @default.
- W2282383970 hasPrimaryLocation W22823839701 @default.
- W2282383970 hasRelatedWork W1964569358 @default.
- W2282383970 hasRelatedWork W1972989483 @default.
- W2282383970 hasRelatedWork W1977030602 @default.
- W2282383970 hasRelatedWork W2014776579 @default.
- W2282383970 hasRelatedWork W2021263266 @default.
- W2282383970 hasRelatedWork W2027284031 @default.
- W2282383970 hasRelatedWork W2043539242 @default.
- W2282383970 hasRelatedWork W2059978259 @default.
- W2282383970 hasRelatedWork W2068784750 @default.
- W2282383970 hasRelatedWork W2078856705 @default.
- W2282383970 hasRelatedWork W2104455732 @default.
- W2282383970 hasRelatedWork W2119034900 @default.
- W2282383970 hasRelatedWork W2126021575 @default.