Authors: Abdul Al Atem, Victor Bratus, Bruno Canut, Jeremie Lefevre, Gérard Guillot, Jean Marie Bluet
Abstract: Combined Photoluminescence (PL) and electron paramagnetic resonance (EPR) spectroscopy have been used to characterize cubic silicon carbide (3C-SiC) samples after electron and proton irradiation. We have studied the effects of the thermal annealing (500-1000°C) on the PL intensity in the visible and the near infra-red (NIR) ranges and identified the point defects formation after these two processes of irradiation.
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Authors: Nada Habka, Véronique Soulière, Jean Marie Bluet, Maher Soueidan, Gabriel Ferro, Bilal Nsouli
Abstract: We report an optical study of 3C-SiC layers grown on 6H-SiC substrates by VLS
mechanism using a Si-Ge melt. The photoluminescence and μ-Raman results show a clear and
significant incorporation of germanium in the layers from the melt. A photoluminescence emission
attributed to Ge related transitions is observed in the infrared region. μ-Raman spectra exhibit two
peaks related to the Ge-Ge and Si-Ge bonds. From the characteristics of these Raman peaks, it was
found that the amount of Ge incorporated inside the 3C layers increases with increasing Ge content
of the melt. This has been verified by Particle-Induced X-rays Emission (PIXE) measurements
which gave a Ge concentration varying from ~ 1x1019 to ~ 1x1020 at.cm-3. All these results suggest
that Ge incorporates in the VLS grown 3C layers by forming Si-Ge-(C) nanoclusters.
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Authors: Jacques Botsoa, Jean Marie Bluet, Vladimir Lysenko, Olivier Marty, Daniel Barbier, Gérard Guillot
Abstract: Photoluminescence properties of a freestanding nanoporous SiC layer obtained from bulk
6H-SiC substrate as well as SiC nanopowder consisting of numerous separated nanoparticles has
been investigated. The nanoporous SiC layer is obtained by UV radiation assisted electrochemical
etching of the 6H-SiC wafer and the SiC nanopowder is formed by mechanical grinding of the
nanoporous SiC free layer. A comparison of low temperature PL spectra of the SiC nanostructures
and initial SiC bulk substrate has been performed. The evolution of PL spectra of the SiC
nanostructures with respect to their surface states and excitation laser power has been studied. In
particular, the well pronounced high energy tail above the excitonic bandgap in the PL spectra of
the nanostructured SiC is attributed to quantum confinement effects. The strong PL signal obtained
below the bandgap is explained by radiative transitions involving surface states, N-Al donoracceptor
recombination levels and deep levels corresponding to volume defects in the SiC
nanocrystallites.
407
Authors: Nada Habka, Véronique Soulière, Jean Marie Bluet, Maher Soueidan, Gabriel Ferro, Yves Monteil
Abstract: We report an optical investigation of cubic Silicon Carbide (3C-SiC) layers grown on
6H-SiC substrates by Chemical Vapour Deposition and Vapour-Liquid-Solid mechanism. Micro-
Infrared reflectance ('-IR), micro-Raman ('-Raman) and low temperature photoluminescence
spectroscopies were used for the characterisation of such layers. '-IR measurements showed
unusual optical behaviour of 3C-SiC layers. The difference of refraction index between the 3C-SiC
film and the 6H-SiC substrate cannot explain this result. The experimental '-IR reflectance
spectrum was modelled by introducing a thin (thickness ≤ 0.5 'm) metallic-like (doping ≥ 1020
at.cm-3) interfacial film between the layer and the substrate. The photoluminescence spectra
revealed the presence of a peak which may be attributed to recombination at the 3C/6H interface.
All these results suggest the presence of a two dimensional electron gas at the interface.
403
Authors: Igor Matko, Bernard Chenevier, Jean Marie Bluet, Roland Madar, Fabrice Letertre, Wahib Saikaly
Abstract: QuaSiC TM substrates can be obtained by transferring a single crystal SiC layer onto a
poly SiC substrate using the Smart Cut TM technology. In order to overcome the difficulty of limited
thickness, an important improvement has been demonstrated, which consists in obtaining thick SiC
structure by growing epitaxial SiC layers on top of transferred layers. The aim of this work is a
structural analysis of such layers by Transmission Electron Microscopy and Photoluminescence.
255
Authors: Maher Soueidan, Gabriel Ferro, Bilal Nsouli, Nada Habka, Véronique Soulière, Ghassan Younes, Khaled Zahraman, Jean Marie Bluet, Yves Monteil
Abstract: Vapor-Liquid-Solid was used for growing boron doped homoepitaxial SiC layers on 4HSiC(
0001) 8°off substrates. Si-based melts were fed by propane (5 sccm) in the temperature range
1450-1500°C. Two main approaches were studied to incorporate boron during growth : 1) adding
elemental B in the initial melt, with two different compositions : Si90B10 and Si27Ge68B5; the growth
was performed at 1500°C; 2) adding B2H6 (1 to 5 sccm) to the gas phase during growth with a melt
composition of Si25Ge75; the growth was performed at 1450°C. In most cases, the growth time was
limited by liquid loss due to wetting on the crucible walls. The longer growth duration (1h) was
obtained when adding B2H6 to the gas phase. In the case of Si90B10 melt, the surface morphology
exhibits large and parallel terraces whereas the step front is more undulated when adding Ge.
Raman and photoluminescence characterizations performed on these layers confirmed the 4H
polytype of the layers in addition to the presence of B which results in a strong B-N donor-acceptor
band. Particle induced γ-ray emission was also used to detect B incorporation inside the grown
layers.
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Authors: Tetyana Nychyporuk, Olivier Marty, Jean Marie Bluet, Vladimir Lysenko, Robert Perrin, Gérard Guillot, Daniel Barbier
Abstract: SiC nanopowder has been formed using an original technological approach based on
grinding of bulk porous SiC nanostructures. The initial porous SiC nanostructures were obtained by
anodization of n+-type 4H-SiC substrate in HF/Ethanol solution under UV illumination. Large
single SiC nanoparticles (~ 30 nm in diameter) constituting the nanopowder have a porous structure
which can be clearly visible. On the other hand, small single SiC nanoparticles (~ 4 nm in diameter)
exhibit a clear crystalline structure. A broad and very intense luminescence band (400 – 900 nm)
provided from the nanopowder corresponds to the radiative processes involving nanoparticle
surface states. A smaller photoluminescence peak centred at 358 nm may correspond to radiative
recombination of the photogenerated excitons confined in the individual and spatially separated 4HSiC
nanoparticles.
763
Authors: Mohamed Trabelsi, Nabil Sghaier, Jean Marie Bluet, Noureddine Yacoubi, Gérard Guillot, Christian Brylinski
Abstract: Our work is focused on the identification of defects responsible for current fluctuations at
the origin of low frequency noise or random telegraphic signals in 4H-SiC MESFETs on semiinsulating
(SI) substrates. We show that devices having instabilities have DC output characteristics
with random discrete fluctuations of the drain current. The RTS noise parameters analysis
(amplitude, high and low state time durations) as a function of temperature and bias voltage
provides the signature of the involved traps (activation energy and cross section both for emission
and capture). From the power spectral density of the drain current noise (PSD) we have measured
the cut-off frequency of a single trap even at very low frequencies (from 0.1 Hz) and we propose
that the noise responsible of RTS fluctuations is a generation-recombination noise. Finally, it is
shown that the frequency analysis of the random telegraphic signal is a well-suited tool for the study
of single defects in very small devices.
1251
Authors: Guy Chichignoud, Laurent Auvray, Elisabeth Blanquet, Mikhail Anikin, Etienne Pernot, Jean Marie Bluet, Patrick Chaudouët, Michel Mermoux, Catherine Moisson, Fabrice Letertre, Michel Pons, Roland Madar
Abstract: The transfer by wafer-bonding of single-crystalline SiC thin films to a
polycrystalline SiC support to obtain a “quasi-wafer” is an attractive way for lowering the
cost of silicon carbide wafers. Such a process needs high quality polycrystalline substrates,
with controlled and high-level bulk properties (thermal conductivity, electrical resistivity) and
with very low surface roughness and surface bowing. Currently, polycrystalline SiC wafers
which are available are siliconized SiC or CVD processed SiC wafers. Siliconized ceramic
wafers are very heterogeneous (mixture of 3C, 6H, 15R and silicon), while CVD ones are of
better quality (homogeneous and textured 3C). However neither the siliconized SiC nor the
CVD SiC can be CMP polished with low roughness over large dimension. In this paper,
wafers with large and textured grains (> 1cm) are processed and characterized. The polishing
of such structures is studied and optimized to obtain low surface roughness. To meet these
requirements high temperature processes used for single crystal growth were selected.
Structural investigations performed on the grown ingots showed an important influence of the
used seed since no preferential crystallographic orientation was observed during the growth.
The final polishing quality was of high level but step heights were observed between grains.
71
Authors: Jean Marie Bluet, M. Gassoumi, I. Dermoul, F. Chekir, H. Maaref, Gérard Guillot, Erwan Morvan, Christian Dua, Christian Brylinski
Abstract: Conductance DLTS measurements have been performed on 4H-SiC MESFETs. A broad band due to electron emission by different levels is observed. An additional “hole-like” level with activation energy of 0.9 eV is obtained in linear regime but not in saturation regime. From the results, it is proposed that this “hole-like” signal is due to capture of electron present at a conductive
SiC/SiO2 interfacial layer.
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