2011
DOI: 10.12693/aphyspola.119.203
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Small-Signal Characterization of FET/HEMT for Terahertz Applications

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Cited by 3 publications
(1 citation statement)
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“…2a curves x i = 13 and 38 nm) stimulates weakly the different modes; • The 20 THz resonance is strongly stimulated by an excitation positioned in the drain region (x i = 263 and 288 nm); indeed, a 3D plasma oscillation appears here, due to the long-range interaction of the Coulomb forces leading to mutual oscillations of the blocks of electrons with different carrier concentrations n and n + [9]; the oscillation occurring in the source region is not visible at the drain since this long-range interaction is suppressed by the gated region; • The perturbations located in the n central region induce strong resonances at f = 2 and 6 THz; they result from the excitation of 2D plasma modes of free-carrier oscillations in the gated and ungated parts of the channel; these oscillations describe various spatial modes appearing during the recharge of the distributed capacitance between the gate and channel [10], [11]. On can also remark that a perturbation applied around the middle of the channel (x i = 138 and 163 nm) excites weakly the fundamental mode but strongly the second one.…”
Section: Local Spectral Densitiesmentioning
confidence: 99%
“…2a curves x i = 13 and 38 nm) stimulates weakly the different modes; • The 20 THz resonance is strongly stimulated by an excitation positioned in the drain region (x i = 263 and 288 nm); indeed, a 3D plasma oscillation appears here, due to the long-range interaction of the Coulomb forces leading to mutual oscillations of the blocks of electrons with different carrier concentrations n and n + [9]; the oscillation occurring in the source region is not visible at the drain since this long-range interaction is suppressed by the gated region; • The perturbations located in the n central region induce strong resonances at f = 2 and 6 THz; they result from the excitation of 2D plasma modes of free-carrier oscillations in the gated and ungated parts of the channel; these oscillations describe various spatial modes appearing during the recharge of the distributed capacitance between the gate and channel [10], [11]. On can also remark that a perturbation applied around the middle of the channel (x i = 138 and 163 nm) excites weakly the fundamental mode but strongly the second one.…”
Section: Local Spectral Densitiesmentioning
confidence: 99%