PHEMT saturation velocity and mobility is taken 1.5 ϫ 10 7 cm/sec and 7000 cm 2 /V ⅐ sec, respectively.
CONCLUSIONAn analytical noise modeling is performed using an accurate charge-control model to evaluate the small-signal parameters and noise properties of HEMT and PHEMT. This model shows improved behavior of transconductance and gate-to-source capacitance near the threshold region; hence, the calculated curves of minimum noise figure F min and minimum noise temperature T min show good matching with the experimental data. Excellent agreement with the experimental results ensures the validity of the proposed model. The effects of gate length and donor layer thickness upon noise performance are also studied, which suggest that noise performance improves with reducing gate length and increasing thickness, however, one needs to maintain the aspect ratio in order to avoid short-channel effects.
ACKNOWLEDGMENTThe
One means of converting the port conditions of a magic-tee into those of a 908 hybrid is to introduce external sections of waveguide at the symmetrical H-plane output ports having the necessary 908 phase difference. The purpose of this article is to describe a number of realizations of such differential phase shifters (DPS), including an exact synthesis procedure not requiring computer optimization. A typical design consists of a capacitively loaded waveguide for one section and an essentially inductive waveguide for the other. The latter is simply a uniform waveguide of reduced width when compared with that of the capacitive section. An example capacitive ridge DPS exhibits a maximum phase error of 628 over a 20% bandwidth in WR75 waveguide with a return loss of better than 40 dB and an insertion loss <0.06 dB.
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