Matches in SemOpenAlex for { <https://semopenalex.org/work/W3153024090> ?p ?o ?g. }
- W3153024090 endingPage "934" @default.
- W3153024090 startingPage "931" @default.
- W3153024090 abstract "In vacuum electronics, the influence of the uniformity of electron beams on the performance of two- or multi-beam devices is a key scientific problem in the development of compact, high power millimeter-wave and terahertz (THz) sources. In this letter, we focus on this problem in extended interaction oscillators (EIOs) and propose a tractable extended resonant circuit that has no requirement for the uniformity of beams. The circuit design builds up a TM <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>13</sub> mode mechanism to support two nonuniform beams, based on maintaining the same electromagnetic characteristics of conventional resonant circuits used in single-beam EIOs. To verify this idea, we designed and simulated a 0.22-THz EIO with the proposed circuit. As the current of one beam is I <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>1</sub> and that of another beam is increased from 0 to 4I <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>1</sub> , the EIO has shown the behavior of linearly increasing the output power and then becoming saturated through particle-in-cell (PIC) simulations. The ideal case is the currents of the two beams are the same at the same voltage to drive the EIO. This case can reduce the high current density required for start oscillation in single-beam EIOs and obtain high power. Simulation results show that the power of 0.22-THz wave over 1.32 kW is obtained using double beams at 22.2 kV and each current of 0.25 A." @default.
- W3153024090 created "2021-04-26" @default.
- W3153024090 creator A5011153224 @default.
- W3153024090 creator A5030610339 @default.
- W3153024090 creator A5039753466 @default.
- W3153024090 creator A5054433234 @default.
- W3153024090 creator A5057664591 @default.
- W3153024090 creator A5076055846 @default.
- W3153024090 creator A5078249204 @default.
- W3153024090 creator A5080443891 @default.
- W3153024090 date "2021-06-01" @default.
- W3153024090 modified "2023-10-16" @default.
- W3153024090 title "Tractable Resonant Circuit With Two Nonuniform Beams for a High-Power 0.22-THz Extended Interaction Oscillator" @default.
- W3153024090 cites W1553866613 @default.
- W3153024090 cites W1964257685 @default.
- W3153024090 cites W1967643181 @default.
- W3153024090 cites W1975674477 @default.
- W3153024090 cites W2072633836 @default.
- W3153024090 cites W2090083474 @default.
- W3153024090 cites W2106251071 @default.
- W3153024090 cites W2111520621 @default.
- W3153024090 cites W2114613949 @default.
- W3153024090 cites W2125194290 @default.
- W3153024090 cites W2166663796 @default.
- W3153024090 cites W2180018597 @default.
- W3153024090 cites W2467339192 @default.
- W3153024090 cites W2512590682 @default.
- W3153024090 cites W2531136231 @default.
- W3153024090 cites W2567862405 @default.
- W3153024090 cites W2615813585 @default.
- W3153024090 cites W2792178484 @default.
- W3153024090 cites W2810141020 @default.
- W3153024090 cites W2901260519 @default.
- W3153024090 cites W2904663087 @default.
- W3153024090 cites W2905545533 @default.
- W3153024090 cites W2948489559 @default.
- W3153024090 cites W2950946522 @default.
- W3153024090 cites W2963558869 @default.
- W3153024090 cites W2994762004 @default.
- W3153024090 cites W3018647890 @default.
- W3153024090 cites W3093864856 @default.
- W3153024090 cites W3109056438 @default.
- W3153024090 cites W3112821762 @default.
- W3153024090 cites W4238783456 @default.
- W3153024090 doi "https://doi.org/10.1109/led.2021.3072848" @default.
- W3153024090 hasPublicationYear "2021" @default.
- W3153024090 type Work @default.
- W3153024090 sameAs 3153024090 @default.
- W3153024090 citedByCount "12" @default.
- W3153024090 countsByYear W31530240902021 @default.
- W3153024090 countsByYear W31530240902022 @default.
- W3153024090 countsByYear W31530240902023 @default.
- W3153024090 crossrefType "journal-article" @default.
- W3153024090 hasAuthorship W3153024090A5011153224 @default.
- W3153024090 hasAuthorship W3153024090A5030610339 @default.
- W3153024090 hasAuthorship W3153024090A5039753466 @default.
- W3153024090 hasAuthorship W3153024090A5054433234 @default.
- W3153024090 hasAuthorship W3153024090A5057664591 @default.
- W3153024090 hasAuthorship W3153024090A5076055846 @default.
- W3153024090 hasAuthorship W3153024090A5078249204 @default.
- W3153024090 hasAuthorship W3153024090A5080443891 @default.
- W3153024090 hasConcept C107816215 @default.
- W3153024090 hasConcept C119599485 @default.
- W3153024090 hasConcept C120665830 @default.
- W3153024090 hasConcept C121332964 @default.
- W3153024090 hasConcept C127413603 @default.
- W3153024090 hasConcept C134146338 @default.
- W3153024090 hasConcept C163258240 @default.
- W3153024090 hasConcept C168834538 @default.
- W3153024090 hasConcept C184720557 @default.
- W3153024090 hasConcept C45764600 @default.
- W3153024090 hasConcept C49040817 @default.
- W3153024090 hasConcept C62520636 @default.
- W3153024090 hasConceptScore W3153024090C107816215 @default.
- W3153024090 hasConceptScore W3153024090C119599485 @default.
- W3153024090 hasConceptScore W3153024090C120665830 @default.
- W3153024090 hasConceptScore W3153024090C121332964 @default.
- W3153024090 hasConceptScore W3153024090C127413603 @default.
- W3153024090 hasConceptScore W3153024090C134146338 @default.
- W3153024090 hasConceptScore W3153024090C163258240 @default.
- W3153024090 hasConceptScore W3153024090C168834538 @default.
- W3153024090 hasConceptScore W3153024090C184720557 @default.
- W3153024090 hasConceptScore W3153024090C45764600 @default.
- W3153024090 hasConceptScore W3153024090C49040817 @default.
- W3153024090 hasConceptScore W3153024090C62520636 @default.
- W3153024090 hasFunder F4320321001 @default.
- W3153024090 hasFunder F4320335777 @default.
- W3153024090 hasFunder F4320335787 @default.
- W3153024090 hasIssue "6" @default.
- W3153024090 hasLocation W31530240901 @default.
- W3153024090 hasOpenAccess W3153024090 @default.
- W3153024090 hasPrimaryLocation W31530240901 @default.
- W3153024090 hasRelatedWork W1549716197 @default.
- W3153024090 hasRelatedWork W2023543129 @default.
- W3153024090 hasRelatedWork W2163743881 @default.
- W3153024090 hasRelatedWork W2343543068 @default.
- W3153024090 hasRelatedWork W2736258467 @default.
- W3153024090 hasRelatedWork W2899100519 @default.