1980
DOI: 10.1016/0038-1101(80)90070-2
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Effect of mobile space-charge on the small-signal admittance of DDR silicon IMPATTs at high current densities

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Cited by 11 publications
(8 citation statements)
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“…With increasing bias current density from 8.6 × 10 7 to 9.2 × 10 7 A m −2 and corresponding bias current from 136.8 to 146.3 mA, distortion and nonlinearity is observed in the snapshots at each phase angles (ω t = 0, π /2, π , 3 π /2, 2 π ). This is due to the mobile space charge effect at higher current densities [19, 20]. The electric field snapshots exhibit depletion width modulation at large-signal level for 55% voltage modulation (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…With increasing bias current density from 8.6 × 10 7 to 9.2 × 10 7 A m −2 and corresponding bias current from 136.8 to 146.3 mA, distortion and nonlinearity is observed in the snapshots at each phase angles (ω t = 0, π /2, π , 3 π /2, 2 π ). This is due to the mobile space charge effect at higher current densities [19, 20]. The electric field snapshots exhibit depletion width modulation at large-signal level for 55% voltage modulation (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…At !t D /2, the electric field profiles for all junction temperatures become highly punched through due to the high electric field at the peak of the positive half cycle of the oscillation. It is interesting to note that, during the positive half cycle (0 6 !t 6 /2) the electric field profiles distort at higher junction temperatures (T j > 450 K) due to high space charge effect OE18; 19 . At the end of the positive half cycle (!t D ), the electric field profiles repeat themselves (i.e., at !t D 0 and !t D the electric field profiles are same).…”
Section: Large-signal Propertiesmentioning
confidence: 99%
“…The DC and high-frequency simulation method of MITATT devices presented in this paper is free from cut-down assumptions. The aforementioned method takes into account the realistic doping profiles and the effect of mobile space charge (Gibbons, 1973;Sridharan & Roy, 1978, 1980. The realistic electric field dependence of ionisation rates (α n , α p ) and drift velocities (v n , v p ) of charge carriers and other material parameters of silicon at realistic junction temperature of 500 K are taken from the experimental reports available in literature (Canali et al, 1971;Electronic Archive, 2012;Grant, 1973).…”
Section: Simulation Methods To Study the High-frequency Properties Of mentioning
confidence: 99%
“…The first fundamental device equation, i.e. Poisson's equation (Sze, 1981), taking into account the mobile space charge (Gibbons, 1973;Sridharan & Roy, 1978, 1980 in the space charge region of the device is given by:…”
Section: Simulation Methods To Study the DC Properties Of Impatt/mitatmentioning
confidence: 99%
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