EXPERIMENTAL-DETERMINATION OF THE N-P-PARTIAL DENSITY-OF-STATES IN THE CONDUCTION-BAND OF GAN - DETERMINATION OF THE POLYTYPE FRACTIONS IN MIXED-PHASE SAMPLES
M. Katsikini et al., EXPERIMENTAL-DETERMINATION OF THE N-P-PARTIAL DENSITY-OF-STATES IN THE CONDUCTION-BAND OF GAN - DETERMINATION OF THE POLYTYPE FRACTIONS IN MIXED-PHASE SAMPLES, Journal of applied physics, 83(3), 1998, pp. 1437-1445
Hexagonal, cubic, and mixed phase GaN samples grown by molecular beam
epitaxy are studied using near-edge x-ray absorption fine structure (N
EXAFS) spectroscopy. The spectra were recorded at the N-K-edge, at sev
eral angles of incidence. It is shown that the N-K-edge NEXAFS spectra
, which are proportional to the p-partial density of states in the con
duction band, are characteristic of the cubic or hexagonal structure o
f the examined crystal. The spectra of the cubic sample do not depend
on the angle of incidence (theta), contrary to the spectra of the hexa
gonal sample in which the areas under the NEXAFS resonances depend lin
early on cos(2) theta. From the fitting of the lines A(i) = A + B cos(
2) theta, where A(i) are the areas under the resonances and A and B ar
e constants, the directions of maximum electron charge density with re
spect to the normal to the surface are determined for the hexagonal sa
mple. The energy positions of the absorption edge and the NEXAFS reson
ances in the spectra from the cubic sample are different from those of
the hexagonal sample and in either case are independent of theta. Con
trary to that, the energy positions of the NEXAFS resonances in a mixe
d phase sample have a characteristic angular dependence and shift betw
een the energies corresponding to the cubic and hexagonal polytypes. B
ased on this observation, we propose that the spectrum of the mixed-ph
ase sample can be approximated as the weighted average of the spectra
from the pure cubic and hexagonal samples. From this approximation the
coexisting fractions of alpha- and beta-GaN in a mixed-phase sample a
re determined and they are found in good agreement with results from h
igh resolution transmission electron microscopy and x-ray diffraction.
(C) 1998 American Institute of Physics. [S0021-8979(98)02603-6].