Studies on the millimeter-wave performance of MITTATs from avalanche transit time phase delay
Citations
20 citations
Cites background from "Studies on the millimeter-wave perf..."
...A comprehensive technique to simulate the static (DC) and small-signal (S-S) characteristics of IMPATT devices based on driftdiffusion model was first reported by Roy et al. in the years 1979 and 1985, respectively (Roy, Banerjee, & Pati, 1985; Roy, Sridharan, Ghosh, & Pal, 1979)....
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...R(x,ω) vs. x and X(x,ω) vs. x for a particular ω) in the active region of the device can be obtained (Acharyya et al., 2011b)....
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...Since the electrons in the valance band have no available quantum states in the conduction band for tunnelling within the region 0 ≤ x ≤ xL, the tunnelling generation rate of holes is zero; similarly, within the region xR ≤ x ≤ W no empty states are available in the conduction band for electron tunnelling; thus, the tunnelling generation rate of electrons is zero (Acharyya & Banerjee, 2012b; Acharyya et al., 2011b; Dash & Pati, 1992)....
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...The relationship between x and x’ is given by: x ¼ x0 1 Eg E 12 for 0 x xj; (9) x ¼ W W x0 1þ Eg EB E 12 for xj x W ; (10) where E is the amount of energy with respect to the bottom of the conduction band on the n-side and Eg is the vertical difference between x and x’ (Acharyya & Banerjee, 2012b; Acharyya, Mukherjee, & Banerjee, 2011b; Dash & Pati, 1992)....
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...Tunnelling-assisted phase distortion between external current and applied voltage is responsible for the aforementioned degradation (Acharyya et al., 2011a; Luy & Kuehnf, 1989)....
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16 citations
12 citations
Cites background or methods from "Studies on the millimeter-wave perf..."
...This noise field is assumed to be due to a noise source γ(x′) located at the space point x′ within the space charge region of the device (Acharyya et al., 2010, 2011a; Dash et al., 1996)....
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...Simulation study of avalanche noise performance of the W-band DDR MITATT diode based on Si under unilluminated condition was earlier reported by the authors (Acharyya et al., 2010, 2011a)....
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...…of primary device equations such as Poisson’s equation, combined carrier continuity equation in the steady state, current density equations and mobile space charge equation subject to suitable boundary conditions as discussed in detail in the earlier papers by the authors (Acharyya et al., 2011b)....
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...…used to solve the above mentioned differential equations involving the real (enr(x,x′)) and imaginary parts (eni(x,x′)) of total noise electric field en(x,x′) simultaneously, subject to appropriate boundary conditions at the depletion layer edges (Acharyya et al., 2010, 2011a; Dash et al., 1996)....
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...This phenomenon is also observed in the study of MITATT mode of operation of IMPATT devices by the author in their earlier reports (Acharyya et al., 2011b, 2011c) and also by some other researchers (Dash & Pati, 1992) earlier....
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2 citations
Cites background from "Studies on the millimeter-wave perf..."
...Impact Avalanche Transit Time (IMPATT) device has emerged as the most suitable solid-state source to generate sufficiently high power in microwave, millimeterwave and terahertz frequencies [1-4]....
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References
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