Microwave Field-Effect Transistors: Theory, Design, and Applications

Chapter 2: GaAs FET Theory-Small Signal

2.1 Introduction

Over twenty years ago the first gallium arsenide transistors which used a diffused-gate structure were reported by Turner et al (1967) giving useful gains in the lower megahertz frequency bands. In 1969 Middel-hoek realized a silicon Metal Semiconductor Field Effect Transistor (MESFET) with a 1 ?m gate length by projection masking which had a maximum frequency of oscillation of 12 GHz (Middelhoek, 1970a, b). This was comparable to the maximum frequency of oscillation, f max, of the best bipolar transistors at that time.

In 1971 a significant step was made by Turner et al, when 1 ?m gate length FETs on GaAs were made having f max equal to 50 GHz and useful gains up to 18 GHz.

The substantial improvement in FET performance over the silicon bipolar transistor is due mainly to two reasons:-

  1. In gallium arsenide the conduction electrons have a six times larger mobility and twice the peak drift velocity of those in silicon (Ruch et al, 1970).

  2. The active layer is grown on a semi-insulating GaAs substrate with resistivity larger than 10 7 ? cm. This compares with a typical value of 30 ? cm for intrinsic silicon.

The first property results in lower parasitic resistances, larger transconductances and shorter electron transit times.

The second property results in lower gate-bonding pad parasitic capacitance when the gate pad is on the semi-insulating (SI) substrate.

By the early 1970's it was clear that the gallium arsenide MESFET could be used...

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