Authors: Mary Ellen Zvanut, G. Ngetich, H.J. Chung, A.Y. Polyakov, Marek Skowronski, N.Y. Garces, E.R. Glaser
Abstract: The understanding of the structure and associated defect level of point defects in SiC is
important because the material is to be used both as a semiconductor and semi-insulator.
Production of the latter is achieved by compensation of unavoidable impurities using defects that
require more energy for ionization than the unintentional donors or acceptors. The purpose of the
present work is to measure the defect energy level of one center in high resistivity 4H SiC using
photo-induced electron paramagnetic resonance (photo-EPR). The center is identified as SI-5, an
EPR signal that others have attributed to the negative charge state of the carbon vacancy-carbon
antisite pair, −
C Si V C . Samples containing this defect exhibit two different photo thresholds, which
depend on the resistivity activation energy, Ea. For samples with Ea less than 0.8 eV, a photothreshold
at 0.75+/- 0.05 eV is observed, but for those with Ea greater than 0.8 eV, the threshold is
between 2 and 2.5 eV. Previous work focused on the former case. Here, the SiC substrates with the
larger Ea are emphasized, showing that the photo-threshold likely measures the neutral to negative
defect level, − / 0
C Si V C .
385
Authors: Mary Ellen Zvanut, Hun Jae Chung, A.Y. Polyakov, Marek Skowronski
Abstract: Halide chemical vapor deposition (HCVD) allows for rapid growth while maintaining
the purity afforded by a CVD process. While several shallow and deep defect levels have been
identified in 6H HCVD substrates using electrical techniques, here we examine several different
point defects found in 4H n-type HCVD SiC using electron paramagnetic resonance (EPR)
spectroscopy. One spectrum, which exhibits axial symmetry and broadens upon heating, may
represent a collection of shallow defects. The other prominent defect has the g tensor of the
negatively charged carbon vacancy, but additional hyperfine lines suggest a more complex center.
The role of these defects is not yet determined, but we note that the concentrations are similar to
those found for the electrically detected defect levels, making them a reasonable source of
electrically active centers.
473
Authors: Hun Jae Chung, Sung Wook Huh, A.Y. Polyakov, Saurav Nigam, Qiang Li, J.R. Grim, Marek Skowronski, E.R. Glaser, W.E. Carlos, Jaime A. Freitas, Mark A. Fanton
Abstract: Undoped 6H- and 4H-SiC crystals were grown by Halide Chemical Vapor Deposition
(HCVD). Concentrations of impurities were measured by various methods including
secondary-ion-mass spectrometry (SIMS). With increasing C/Si ratio, nitrogen concentration
decreased and boron concentration increased as expected for the site-competition effect. Hall-effect
measurements on 6H-SiC crystals showed that with the increase of C/Si ratio from 0.06 to 0.7, the
Fermi level was shifted from Ec-0.14 eV (nitrogen donors) to Ev+0.6 eV (B-related deep centers).
Crystals grown with C/Si > 0.36 showed high resistivities between 1053 and 1010 4cm at room
temperature. The high resistivities are attributed to close values of the nitrogen and boron
concentrations and compensation by deep defects present in low densities.
625
Authors: E.R. Glaser, B.V. Shanabrook, W.E. Carlos, Hun Jae Chung, Saurav Nigam, A.Y. Polyakov, Marek Skowronski
Abstract: We have employed low-temperature photoluminescence to estimate the total residual N
concentration in semi-insulating (SI) SiC substrates where all N shallow donors are compensated in
the dark. The ratio of the nitrogen-bound exciton line (Qo) to the free excitonic emission (I77) as a
function of excitation power density (Pexc) was tracked for several SI 4H-SiC samples with varying
residual N concentration (~ 7x1014 – 5.2x1016 cm-3). Most notably, a linear relationship was found
between Qo/I77 and [N] for [N] < 1x1016 cm-3 while a sub-linear behavior was observed for samples
with higher N levels. This technique should be particularly valuable to map [N] where the levels
are close to or below the present SIMS detection limit of ~ 5-7 x 1014 cm-3. Results obtained for a
limited number of low n-type and SI 6H-SiC substrates are also presented.
613
Authors: N.Y. Garces, W.E. Carlos, E.R. Glaser, Sung Wook Huh, Hun Jae Chung, Saurav Nigam, A.Y. Polyakov, Marek Skowronski
547
Authors: Sung Wook Huh, A.Y. Polyakov, Hun Jae Chung, Saurav Nigam, Marek Skowronski, E.R. Glaser, W.E. Carlos, Mark A. Fanton, N.B. Smirnov
Abstract: Deep electron and hole traps were studied in a series of high purity 6H-SiC single crystals
grown by Halide Chemical Vapor Deposition (HCVD) method at various C/Si flow ratios and at
temperatures between 2000 oC and 2100 oC. Characterization included Low Temperature
Photoluminescence (LTPL), Deep Level Transient Spectroscopy (DLTS), Minority Carrier Transient
Spectroscopy (MCTS), and Thermal Admittance Spectroscopy (TAS) measurements. Concentrations
of all deep traps were shown to strongly decrease with increased C/Si flow ratio and with increased
growth temperature. The results indicate that the majority of deep centers in 6H-SiC crystals grown by
HCVD are due to native defects or complexes of native defects promoted by Si-rich growth
conditions. The observed growth temperature dependence of residual donor concentration and traps
density is explained by increasing the effective C/Si ratio at higher temperatures for the same nominal
ratio of C and Si flows.
497
Authors: Sung Wook Huh, Joseph J. Sumakeris, A.Y. Polyakov, Marek Skowronski, Paul B. Klein, B.V. Shanabrook, Michael J. O'Loughlin
Abstract: Carrier lifetimes and the dominant electron and hole traps were investigated in a set of
thick (9-104mm) undoped 4H-SiC epitaxial layers grown by CVD homoepitaxy. Deep trap spectra
were measured by deep level transient spectroscopy (DLTS) with electrical or optical injection,
while lifetimes were measured by room temperature time-resolved photoluminescence (PL). The
main electron traps detected in all samples were due to Ti, Z1/Z2 centers, and EH6/EH7 centers. Two
boron-related hole traps were observed with activation energies of 0.3 eV (boron acceptors) and 0.6
eV (boron-related D centers). The concentration of electron traps decreased with increasing layer
thickness and increased toward the edge of the wafers. PL lifetimes were in the 400 ns-1800 ns
range with varying injection and generally correlated with changes in the density of Z1/Z2 and to a
lesser extent the EH6/EH7 electron traps. However, the results of DLTS measurements on p-i-n
diode structures suggest that the capture of injected holes is much more efficient for the Z1/Z2 traps
compared to the EH6/EH7 centers making the Z1/Z2 more probable candidates for the role of
lifetime killers. A good fit of the thickness dependence of the measured lifetimes to the usual
analytical form was obtained assuming that Z1/Z2 is the dominant hole recombination center and
that the surface recombination velocity was 2500 cm/sec.
493
Authors: Mark A. Fanton, Qiang Li, A.Y. Polyakov, R.L. Cavalero, R.G Ray, B.E. Weiland, Marek Skowronski
Abstract: The effects of H2 addition to the growth ambient during physical vapor transport
(PVT) growth of 6H and 4H SiC were investigated using SIMS, DLTS and Hall effect
measurements. Using this hybrid physical-chemical vapor transport (HPVT) approach, boules were
grown using Ar-H2 and He-H2 mixtures with H2 concentrations up to 50 at%. Thermodynamic
modeling suggests that addition of H2 improves the carbon transport in HPVT compared to standard
PVT. This should lead to a substantial decrease in the concentration of residual N donors and the
concentration of electron traps. This is confirmed by the experimental results. As expected, the
source transport rate increased as H2 was added to the growth environment due to increased C
transport. The background nitrogen concentration and the free electron density decreased
significantly with increasing H2 concentration. The formation of electron traps (activation energies
of 0.4 eV, 0.6-0.65 eV, 0.7 eV, 0.9 eV and 1 eV) was also strongly suppressed. These changes were
observed for H2 concentrations as low as 4 at%. The decreased N concentration improves the
ability to produce high resistivity SiC material, and for H2 concentrations as high as 10-25%, the
very first wafers cut from the seed end of the boules have a resistivity exceeding 106 cm.
103
Authors: Qiang Li, A.Y. Polyakov, Marek Skowronski, Edward Sanchez, Mark J. Loboda, Mark A. Fanton, Timothy Bogart, Rick D. Gamble, N.B. Smirnov, Yuri Makarov
Abstract: For undoped 6H-SiC boules grown by physical vapor transport the variations of resistivity,
of the type and density of deep electron and hole traps, and of the concentration of nitrogen and boron
were studied as a function of position in the cross section normal to the growth axis and along the
growth direction. It was observed that the concentrations of all deep electron and hole traps decreased
when moving from seed to tail of the boule and from the center to the edge of the wafers. Modeling of
the growth process suggests that the C/Si ratio increases in a similar fashion and could be responsible
for observed changes. We also discuss the implications of such stoichiometry changes on
compensation mechanisms rendering the crystals semi-insulating and on electrical uniformity of
SI-SiC wafers.
51
Authors: Saurav Nigam, Hun Jae Chung, Sung Wook Huh, J.R. Grim, A.Y. Polyakov, Mark A. Fanton, B.E. Weiland, David Snyder, Marek Skowronski
Abstract: Growth rates and relative stability of 6H- and 4H-SiC have been studied as a function of
growth conditions during Halide Chemical Vapor Deposition (HCVD) process using silicon
tetrachloride, propane and hydrogen as reactants. The growth temperature ranged from 2000 to 2150
oC. Silicon carbide crystals were deposited at growth rates in the 100-300 μm/hr range in both
silicon- and carbon-supply limited regimes by adjusting flows of all three reactants. High resolution
x-ray diffraction measurements show that the growth on Si-face of 6H- and C-face of 4H-SiC
substrates resulted in single crystal 6H- and 4H-SiC polytype, respectively. The growth rate results
have been interpreted using thermodynamic equilibrium calculations.
27