1968
DOI: 10.1109/proc.1968.6786
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An efficient multiresonant avalanche diode oscillator in the 1.5 to 11 GHz range

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Cited by 15 publications
(4 citation statements)
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“…The ionization coefficients for electrons and holes are assumed to be equal and represented by where A=3.9 x IO3 cm-1, and X=5*4 x 10-6 cm V-1. This is in good agreement with experimental data (Logan and Sze 1966) and the approximation of Sze and Gibbons (1966) for field values of interest.…”
Section: A Model For Gaassupporting
confidence: 91%
See 1 more Smart Citation
“…The ionization coefficients for electrons and holes are assumed to be equal and represented by where A=3.9 x IO3 cm-1, and X=5*4 x 10-6 cm V-1. This is in good agreement with experimental data (Logan and Sze 1966) and the approximation of Sze and Gibbons (1966) for field values of interest.…”
Section: A Model For Gaassupporting
confidence: 91%
“…However, Prager et al (1967) have reported a new mode of oscillation in silicon, differing appreciably from the normal IMPATT mode by giving much greater efficiencies ranging up to 43 % and occurring at slightly lower frequencies. Similar results have been obtained for germanium avalanche diodes by Johnston et al (1968) and for silicon by Snapp and Hoefflinger (1968). Theories for highefficiency oscillations have recently been given by Chlorfeine et al (1969) and by DeLoach and Scharfetter (1970) in terms of a rapid avalanche transient which leaves behind a trapped plasma.…”
Section: Introductionsupporting
confidence: 80%
“…While this technology is well developed in Si and GaAs (see e.g. [10][11][12]), GaN-based IMPATT diodes promise to offer exceptional levels of performance. Recent demonstrations of IMPATT-based oscillations have been achieved [13][14][15].…”
Section: Exploitation Of Impact Ionizationmentioning
confidence: 99%
“…Avalanche diodes of the Impatt type have been vastly improved in efficiency, with efficiencies up to 40% demonstrated [Johnston and Scharietter, 1968], and operation over three octaves (1.5-11 GHz), with efficiencies in the 3 to 20% range [Snapp and Hoeffiinger, 1968]. Important developments in Gunn devices have included the broad electronic tuning of up to 10% with varactor diodes and octave tuning using a YIG sphere [Omori, 1969] Superconducting tunneling at Josephson junctions has been used for millimeter-wave mixing ] and infrared detection , and this technique has promise for subnanosecond computer switching applications [Matisoo, 1966].…”
Section: [1968b]mentioning
confidence: 99%