Authors: Jessica Eid, Jean Louis Santailler, Bernard Ferrand, Guy Rolland, Michel Burdin, R. Lewandowska, Jean Camassel
Abstract: We report the effect of changing the growth conditions in the case of bulk 3C-SiC
crystals grown by the Travelling Zone Method when the seed is placed on the top graphite rod.
First, we investigated the effect of changing the temperature gradient and the cooling ramp. Next
we studied the effect of changing the seed polytype and misorientation. Every time, working in the
1700 °C temperature range, the grown polytype was 3C. From X-ray analysis we evidenced a better
hetero-epitaxial relationship between the seed and layer when a low misorientation angle was used.
Better quality and homogeneity were obtained on the first 500 .m of the layer and, beyond this
thickness, micro-Raman measurements show that the effect of solvent (Si) incorporation is not yet
fully under control.
29
Authors: Masataka Satoh, H. Matsuo
Abstract: The Schottky barrier height (SBH) of Al, Ti, Au, and Ni contacts to n- and p-type 3C-SiC
is investigated by means of I-V and C-V measurements. All metal contacts to n- (net donor
concentration: 1.0 x 1016 /cm3) and p-type (net acceptor concentration: 4 x 1016 /cm3) 3C-SiC show
the rectifying I-V characteristics except for Al contact to n-type 3C-SiC. Only Al contact to n-type
3C-SiC shows the ohmic characteristics. As the work function of metal is increased from 4.3 (Ti) to
5.2 (Ni) eV, SBH for n-type 3C-SiC is increased from 0.4 to 0.7 eV and SBH for p-type 3C-SiC is
decreased from 2.2 to 1.8 eV. The small change of SBH for 3C-SiC may be correlated to the crystal
orientation and the defects on the surface of 3C-SiC.
923
Authors: Philip G. Neudeck, David J. Spry, Andrew J. Trunek
Abstract: This paper reports on initial fabrication and electrical characterization of 3C-SiC p+n
junction diodes grown on step-free 4H-SiC mesas. Diodes with n-blocking-layer doping ranging
from ~ 2 x 1016 cm-3 to ~ 5 x 1017 cm-3 were fabricated and tested. No optimization of junction edge
termination or ohmic contacts was employed. Room temperature reverse characteristics of the best
devices show excellent low-leakage behavior, below previous 3C-SiC devices produced by other
growth techniques, until the onset of a sharp breakdown knee. The resulting estimated breakdown
field of 3C-SiC is at least twice the breakdown field of silicon, but is only around half the
breakdown field of <0001> 4H-SiC for the doping range studied. Initial high current stressing of 3C
diodes at 100 A/cm2 for more than 20 hours resulted in less than 50 mV change in ~ 3 V forward
voltage.
1335
Authors: B. Friedel, Siegmund Greulich-Weber
Abstract: We have investigated the growth of SiC, following a modified sol-gel process,
which not only allows the realization of 3D photonic bandgap materials but also is useful for
various SiC applications like templates in medicine or filters in harsh environment. Depending
on the sol-gel annealing procedure one obtains macro-porous SiC, amorphous SiC, or
from nano to micrometer-sized 3C-SiC single crystals. At low annealing temperatures preferably
nanowires are grown. Via various sol-gel-annealing procedures we are able to prepare
single crystals with sizes ranging from several nm up to several 100 %m, while the resulting
polytype only depends on the annealing temperature available. Not only for photonic applications
useable procedures for doping with shallow level donors and acceptors as well as with
deep level defects are essential. We show that controlled doping is possible either during the
sol-gel preparation or via the gas phase during the following annealing procedure.
759
Authors: Gabriel Ferro, Efstathios K. Polychroniadis, D. Panknin, Wolfgang Skorupa, J. Stoemenos, Yves Monteil
Abstract: The epitaxial relationship of Si deposited on 3C-SiC was studied using both free standing
3C-SiC(100) material from Hoya and 3C-SiC thin layers deposited on Si(100) as substrates. The
conditions of Si growth were varied depending on the substrate. When Si is deposited at 1000°C on
(001) 3C-SiC, it is in perfect epitaxial relation with the SiC layer [100]Si//[100]SiC and
[001]Si//[001]SiC. After a 20 ms flash lamp pulse on the same sample, which has the effect of fast
melting of the Si top layer only, the defects in the Si are eliminated. Using free standing 3C-SiC, the
deposition temperature was not limited by the Si melting point so that it was fixed at 1500°C in
order to form a set of Si liquid droplets on the surface with diameters ranging from 5 to 20 μm.
Surprisingly more than 60% of the Si droplets exhibit the epitaxial relation [110]Si//[001]SiC and
[111]Si//[110]SiC after crystallization. The occurrence of this epitaxial relationship can be understood
in terms of lattice mismatch reduction from 20% to 18.3%. The conditions of crystallization, most
probably the cooling rate, seem to have a strong effect on Si orientation.
1563
Authors: Joerg Pezoldt, Thomas Kups, Petia Weih, Thomas Stauden, Oliver Ambacher
Abstract: 3C-(Si1-xC1-y)Gex+y ternary alloys were grown on 8.5° off axis 4H-SiC substrates by solid
source molecular beam epitaxy in a temperature range between 750°C and 950°C. Energy dispersive
X-ray (EDX) analysis revealed a decrease of the Ge incorporation versus substrate temperature. This
effect is due to the fixed Si/Ge ratio during the epitaxial growth. The Ge distribution within the
grown epitaxial layers was found to be nearly homogeneous. The investigations by atomic location
by channeling enhanced microanalysis allowed the conclusion that Ge is located mainly at Si lattice
sites.
1559
Authors: Adolf Schöner, Mietek Bakowski, Per Ericsson, Helena Strömberg, Hiroyuki Nagasawa, Masayuki Abe
Abstract: Vertical DMOSFET devices with varying size from single cell to 3x3 mm2 large devices
have been realized. The investigated devices had hexagonal and square unit cell designs with 2 $m
and 4 $m channel length. The p-body was aluminum implanted and the source was nitrogen or
phosphorus implanted. Low temperature Ti/W contacts were evaluated.
1273
Authors: Donat J. As, S. Potthast, J. Schörmann, S.F. Li, K. Lischka, Hiroyuki Nagasawa, Masayuki Abe
Abstract: Cubic GaN, AlxGa1-xN/GaN and InyGa1-yN/GaN multiple quantum well (MQW) layers
were grown by plasma assisted molecular beam epitaxy on 200 &m thick free standing 3C-SiC
substrates. The influence of the surface roughness of the 3C-SiC substrates and the influence of
metal coverage during growth are discussed. Optimum growth conditions of c-III nitrides exist,
when a one monolayer Ga coverage is formed at the growing surface. The improvement of the
structural properties of cubic III-nitride layers and multilayers grown on 3C-SiC substrates is
demonstrated by 1 μm thick c-GaN layers with a minimum x-ray rocking curve width of 16 arcmin,
and by c-AlGaN/GaN and c-InGaN/GaN MQWs which showed up to five satellite peaks in X-ray
diffraction, respectively.
1489
Authors: Zhe Chuan Feng, C.W. Huang, W.Y. Chang, Jie Zhao, Chin Che Tin, Wei Jie Lu, W.E. Collins
Abstract: We have performed a combined investigation of experiment and theory on the infrared
reflectance from cubic SiC grown on Si by chemical vapor deposition. A damping behavior of the
interference fringes away from the reststrahlen band and a dip or notch within the “flat top” are
observed from some samples while they does not occur in high quality 3C-SiC/Si samples. The
former is interpreted due to an interfacial transition layer existed between SiC-Si and a rough surface,
while the latter can be demonstrated by a three-component effective medium model.
695
Authors: Dieter Strauch, B. Dorner, A.A. Ivanov, M. Krisch, J. Serrano, Alexey Bosak, Wolfgang J. Choyke, B. Stojetz, Michael Malorny
Abstract: Preliminary results for the phonon dispersion curves of hexagonal 4H-SiC from
experimental inelastic neutron (INS) and X-ray scattering (IXS) are reported and contrasted with
those of cubic 3C-SiC and silicon. The experimental frequencies and scattering intensities are in
excellent agreement with those from first-principles calculations using density-functional methods.
The relative merits of the two experimental techniques and aspects of the density functional
perturbation theory and the so-called frozen phonon method for the determination of the basic
phonon properties are briefly outlined.
689