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Paper Title Page
Abstract: The atomic structure of the 4H-SiC(11 2 0) surface including possible phase
transformations via Si deposition and annealing has been investigated using low energy electron
diffraction (LEED), Auger electron spectroscopy (AES), X-ray photoelectron spectroscopy (XPS)
and atomic force microscopy (AFM). The sample is initially prepared by hydrogen etching before
loading into the ultra-high vacuum system. The sample is then out-gassed to remove oxygen from
the surface. To explore the existence of ordered surface phases, Si is deposited on the sample at
850°C for 15 minutes followed by a series of sequential annealing steps. Throughout this process,
the surface is monitored by LEED, AES and XPS. LEED shows that the surface continuously
maintains a (1×1) periodicity. Yet, two unique and distinguishable (1×1) phases can be identified.
The changes between these phases are clearly demonstrated by the LEED spot intensities.
Simultaneously, the Auger and XPS data show a decrease in Si intensity.
673
Abstract: The morphology and atomic structure of 4H-SiC(1102) and 4H-SiC(1102) surfaces, i.e.
the surfaces found in the triangular channels of porous 4H-SiC, have been investigated using AFM,
LEED and AES. After hydrogen etching the surfaces show steps parallel and perpendicular to the caxis,
yet drastically different morphologies for the two isomorphic orientations. Both surfaces
immediately display a sharp LEED pattern. Together with the presence of oxygen in the AES spectra
this indicates the development of an ordered oxide. Both surfaces show an oxygen free, well ordered
surface after Si deposition and annealing.
677
Abstract: The effects of argon and nitrogen bombardment of 3C-SiC surfaces at acceleration voltages
below 2 keV were studied by stylus profilometry, reflectometry, reflection high energy electron
diffraction and Auger electron spectroscopy (AES). The erosion rate of the SiC surface was
determined. It was found that the sputtering rate for argon was three times higher compared to nitrogen.
AES measurements revealed argon and nitrogen incorporation at a depth of a few nanometers
as well as stoichiometric changes at the same depth scale independent of the acceleration voltage.
In the case of the interaction of nitrogen ions with the 3C-SiC surface the formation of a SiCNalloy
was detected.
685
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
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
Abstract: The coefficient of thermal expansion (CTE) of SiC single crystals is important, in
particular, for both designing device assembly and controlling stress distributions in heteroepitaxial
thin film structures grown onto SiC substrates. We have performed very precise measurements of
the CTEs for SiC single crystals comprising of single 4H polytype PVT-grown in NIPPON Steel
Corporation for a temperature range from 123 K to 473 K using a laser interferometry method. This
method allows us to directly measure the temperature dependent variation in thermal expansion of
the crystal volume with much higher accuracy, and enables us to straightforwardly obtain practical
information of CTE data. Furthermore in order to discuss the CTE behavior for a wider temperature
range the CTEs at higher temperatures up to 1573 K have been also measured using dilatometer
method. The CTE obtained for a nitrogen-doped 4H-SiC single crystal increases continuously from
0.8 ppm/K to 3.1 ppm/K for temperatures of 273 K and 423 K respectively, and further increases to
5.4 ppm/K at 1273 K. We conclude from our data that the CTE variations are likely to be almost
independent of the crystal axis directions of SiC from 123 K up to 1573 K.
699
Abstract: In this paper we combine the use of photo-thermal techniques, Thermal lens (TL)
spectrometry, Photoacoustic and heat capacity measurements to determine the optical path
dependence with temperature (ds/dT) of a polycrystalline 3C-SiC sample. Results obtained for the
polycrystalline sample with the TL technique show that ds/dT is negative at room temperature. This
means that the thermal lens formed in 3C-SiC acts as a divergent lens when light impinges the
sample. Our measurements, demonstrate that photo-thermal techniques can be used to obtain
thermal parameters in circumstances where other techniques cannot be used, for example, in harsh
environments.
703
Abstract: The work deals with the highly important problem of the qualitative temperature
dependence of avalanche breakdown voltage in p-n junctions based on 4H-SiC. As it has been
shown before, the temperature coefficient of avalanche breakdown voltage (TCABV) is negative in
seven SiC polytypes, including 4Н-SiC. This effect has been explained by the Wannier-Stark
localization (WSL). It is worth noting that the plane of the investigated p-n junctions coincided with
the basal plane (0001). However the current SiC device technology prefers 4H-SiC p-n junction
formation on a plane that has 8о disorientation from (0001). This may result in a weakening of the
WSL and, correspondingly, in a positive TCABV. This problem has been elucidated in the present
paper. The photocurrent of 4H-SiC p-n junctions in a strong electric field has been scrutinized, that
has allowed to discover a negative differential conductivity region and it has testified to the WSL
process and negative TCABV.
707