Report
on TMS Workshop on "Doping, Dopants and Carrier Dynamics in Wide Bandgap
Semiconductors" in Copper Mountain Resort, Colorado, April 2-6, 2000
.
This
meeting was sponsored by Office of Naval Research (ONR) and TMS, and organized
by F Schubert, Boston University. The practical arrangements were as usual
handled in an excellent way by Allwood Inc. There were about 50 participants,
the weather was good, and everybody returned back home with an embarrassingly
strong tan.
Acceptor
doping remains an important topic, and was discussed in a number of
contributions. Be is believed to be the shallowest acceptor in GaN, and may
readily be introduced in MBE growth. (It is more hazardous in MOCVD growth).
P-type doping at 2x10
17
cm
-3
was reported with Be doping, with a mobility of 200 cm
2/Vs
at 300 K.
Co-doping
was discussed extensively, it now seems that this technique is becoming
appreciated in the III-N community. The theory of co-doping to improve the
p-type conductivity was reviewed, with applications suggested besides GaN also
for AlN and ZnO. Good p-type material was suggested for C-O co-doped AlN (2C
per O). For ZnO good p-type behavior is expected for N acceptors co-doped with
Al or Ga (e g 2 Al per N). The first experimental results on p-type ZnO seem to
verify these ideas.
Experimental
demonstration of a much improved p-type conductivity for Mg-doped GaN with O
co-doping in MOVPE was given. These results seem to confirm the theoretical
predictions that both the hole activation and the hole mobility are drastically
improved by co-doping at levels up to the 10
20
cm
-3
range. It was also claimed by some authors that the co-doping would increase
the solubility of Mg in GaN. A rumour was around that the latest high power
laser diodes announced by Nichia were made using co-doping in the p-region.
Preliminary
reports were given on a similar role of H in co-doping, i e a substantial
improvement of both Be and Mg p-doping was observed in the presence of atomic H
in MBE growth.
Not
much progress was made on the identification of optical spectra for donors and
acceptors in GaN. To get a definite identification of defect-related spectra
much better material quality is needed, very little can be done with
hetero-epitaxial layers, due to the dislocation-induced broadening of the
spectral linewidth. On topic discussed was the 3.27 eV PL spectrum in GaN,
which is indeed very common in GaN. No final conclusion was given, those
working with Mg doping reassured this spectrum was the Mg acceptor signature.
The same spectrum was observed with C or Si doping, however, or even in undoped
samples grown in an equipment which has never seen Mg! More work is needed
here...
Theoretical
models of the limitations of doping (n-type and p-type) for different wide
bandgap materials was reviewed, in terms of the position of the Fermi level
stabilization energy E
FS.
The ease of doping the material n- or p-type is then determined by the position
of E
FS
vs the band edges for each material. In general strong n-doping requires a
large electron affinity χ, while good p-doping requires a small work
function φ. For a recent literature reference see e g Phys Rev Lett 84,
1232 (2000).
Studies
of donor dopants in GaN and AlGaN under high hydrostatic pressure were
reported. It was previously found that O shows a metastable behavior, i e a
deep state at high Al compositions in AlGaN. It was shown that the shallow Si
donor has in fact a similar behavior, in contrast to most theoretical
predictions. These donors reveal the deep level at high pressures in GaN.
Polarization
doping has been found to be very important for III-N structures. A report was
given of polarization doping of holes in AlGaN/GaN heterostructures. A 2D hole
gas is expected to exist in suitably gated structures, at densities 10
13
cm
-2
or higher. This is of great interest for improvement of the base spreading
resistance in AlGaN/GaN HBT structures. The induced base transistor (IBT)
concept was discussed, based on n-GaN/AlGaN/GaN/n-InAlGaN, where a thin GaN QW
base has been inserted. Such a structure was claimed to be a strong competitor
to a regular HBT structure.
An
interesting approach to improved p-type conductance is the p-type superlattice
doping utilizing the strong polarization fields in AlGaN/GaN systems.
Previously only the improvements in the lateral p conduction in the structure
were reported. New EBIC experiments measuring both the vertical and the lateral
minority carrier diffusion lengths L
D
were reported. A ratio of 2.6 between the lateral and vertical L
D
values was found. This ratio may be reduced by grading the superlattice
structure. The data are relevant for the base conductance of HBTs.
Bo
Monemar
© 2000 The Materials Research Society