396 CHAPTER 8. FIELD EFFECT TRANSISTORS
Design Issues in HFET Technology
DESIGNISSUE NEED METHODOLOGY
- Ohmic contact
resistance
Minimize n+ cap layers, optimized alloying
schemes, ion implantation
- Channel and
access resistance
Minimize Ion implantation, high 2DEG
density-mobility product,
n+ cap layers
- Substrate injection Minimize Quantum well structures, p-type
buffers - Gate leakage Minimize Junction HFETs, insulated gate
structures, gate recess, field plates - Parasitic
capacitances
Minimize Low Κ dielectrics, lateral structures
preferred
- Breakdown voltage Maximize Gate recess structures, high
bandgap materials, field plates - Threshold voltage Control Etch-stop layers, controlled
epitaxial growth
Table 8.1: Overview of technology issues that must be addressed in HFET design.
figure 8.24 along with a band diagram. The access resistance of the HFET is comprised of the
sheet resistance of then+cap layerRn+, the sheet resistance of the 2DEGR 2 DEG,andthe
interchannel resistance posed by the barrier to electron flow between the cap and the channel
Rint(see figure 8.24b). The total resistance can be modeled as a distributed network of all of
these components, as shown schematically in figure 8.24a.
Solutions to reducingRintare to reduce the barrier to electron flow from then+layer to the
2DEG channel, and to reduce the barrier to tunneling. The first is best achieved by increasing the
doping in then+layer so that it is very degenerate, causingEFto rise aboveEC. The second is
achieved by addingn+doping in the AlGaAs layer nearest to the surface, which in turn enhances
the surface electric field and thereby tunneling. A schematic diagram illustrating the benefits of
both these solutions is shown in figure 8.25.
8.7.2 Maximizing 2DEG Conductivity ......................
The 2DEG conductivity in MODFET structuresσis given by
σ=eμnns (8.7.1)