1995
DOI: 10.1049/el:19950390
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140 GHz GaAs double-Read IMPATT diodes

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Cited by 41 publications
(10 citation statements)
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“…Figure 12 shows that the experimental results are in very close agreement with the simulation results for Si DDR IMPATTs which validates the DC and high-frequency simulation technique adopted by the authors and used in this paper. Experimentally obtained RF power output from GaAs DDR IMPATT sources are 1.24 W, 270 and 100 mW at 60, 95 and 144 GHz, respectively (Adlerstein and Chu 1984;Eisele 1989;Tschernitz and Freyer 1995), and the same from InP DDR IMPATT source is 55 mW at 84.8 GHz (Eisele et al 1996). Experimentally obtained power outputs from GaAs and InP IMPATT sources are also shown in Fig.…”
Section: High-frequency Propertiesmentioning
confidence: 75%
“…Figure 12 shows that the experimental results are in very close agreement with the simulation results for Si DDR IMPATTs which validates the DC and high-frequency simulation technique adopted by the authors and used in this paper. Experimentally obtained RF power output from GaAs DDR IMPATT sources are 1.24 W, 270 and 100 mW at 60, 95 and 144 GHz, respectively (Adlerstein and Chu 1984;Eisele 1989;Tschernitz and Freyer 1995), and the same from InP DDR IMPATT source is 55 mW at 84.8 GHz (Eisele et al 1996). Experimentally obtained power outputs from GaAs and InP IMPATT sources are also shown in Fig.…”
Section: High-frequency Propertiesmentioning
confidence: 75%
“…Variation of RF power output ( P RF ) of DDR G‐IMPATT devices (under PCPC mode consisting of N = 10 parallel connected diodes) with operating frequency, considering r α = 1.0 is shown in Figure . The same figure also shows the variations of P RF of IMPATT sources based on Wz‐GaN, 4H‐SiC, type‐IIb diamond, GaAs, InP, and Si with frequency obtained from simulation as well as experimental measurements (where available in literature) . The rate of decrease of the RF voltage with operating frequency is found to be much greater that the rate of increase of the magnitude of the negative conductance with respect to the frequency (| dV rf / df | >> | dG p / df |); that is why the RF power output is bound to decrease with the increase of the operating frequency.…”
Section: Characteristics Of G‐impatt Sourcesmentioning
confidence: 88%
“…In the same figure the simulated and experimentally measured power outputs of IMPATT sources based on Si, GaAs, InP, type-IIb diamond and Wurtzite (Wz)-GaN are also shown. [39][40][41][42][43][44][45][46][47][48] It is interesting to observe from Figure 13 that the power output of ten-element mutually injection locked G-IMPATT source exceeds the power output of most promising Wz-GaN IMPATT source when the frequency of operation increases up to 5.0 THz. Therefore, mutually injection locked N-element (N ≥ 10) G-IMPATT sources operating in PCPC mode is the best choice for generating THz frequencies greater than 5.0 THz.…”
Section: F I G U R Ementioning
confidence: 98%