Didier Chaussende

Dr. Didier Chaussende

Universite Grenoble Alpes, CNRS, Saint Martin d'Heres, France
orcid

Research Focus & Metrics

Academic Career Length

29Years (1998-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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27 October 2010 in Journal of Physics D: Applied Physics
Verified
Journal Article
Closed access
ADA Debelle
A Debelle
LTL Thomé
L Thomé
DDD Dompoint
D Dompoint
ABA Boulle
A Boulle
FGF Garrido
F Garrido
DCDidier Chaussende
Didier Chaussende
6H-SiC and 3C-SiC single crystals were simultaneously irradiated at room temperature with 100 keV Fe ions at fluences up to 4 × 1014 cm−2 (∼0.7 dpa), i.e. up to amorphization. The disordering behaviour of both polytypes has been investigated by means of Rutherford backscattering spectrometry in the channelling mode and synchrotron x-ray diffraction. For the first time, it is experimentally demonstrated that the general damage build-up is similar in both polytypes. At low dose, irradiation induces the formation of small interstitial-type defects. With increasing dose, amorphous domains start to form at the expense of the defective crystalline regions. Full amorphization of the irradiated layer is achieved at the same dose (∼0.45 dpa) for both polytypes. It is also shown that the interstitial-type defects formed during the first irradiation stage induce a tensile elastic strain (up to ∼4.0%) with which is associated an elastic energy. It is conjectured that this stored energy destabilizes the current defective microstructure observed at low dose and stimulates the formation of the amorphous nanostructures at higher dose. Finally, the disorder accumulation has been successfully reproduced with two models (namely multi-step damage accumulation and direct-impact/defect-stimulated). Results obtained from this modelling are compared and discussed in the light of experimental data.

29 October 2013 in Physical Review B
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Journal Article
Open access
CCC. Coletti
C. Coletti
SFStiven Forti
Stiven Forti
APA. Principi
A. Principi
KEK. V. Emtsev
K. V. Emtsev
AZA. A. Zakharov
A. A. Zakharov
USU. Starke
U. Starke
In recent times, trilayer graphene has attracted wide attention owing to its stacking and electric-field-dependent electronic properties. However, a direct and well-resolved experimental visualization of its band structure has not yet been reported. In this paper, we present angle-resolved photoemission spectroscopy data which show with high resolution the electronic band structure of trilayer graphene obtained on α-SiC(0001) and β-SiC(111) via hydrogen intercalation. Electronic bands obtained from tight-binding calculations are fitted to the experimental data to extract the interatomic hopping parameters for Bernal and rhombohedral stacked trilayers. Low-energy electron microscopy measurements demonstrate that the trilayer domains extend over areas of tens of square micrometers, suggesting the feasibility of exploiting this material in electronic and photonic devices. Furthermore, our results suggest that, on SiC substrates, the occurrence of a rhombohedral stacked trilayer is significantly higher than in natural bulk graphite.

6 September 2012 in Physical Review B
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Journal Article
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ADA. Debelle
A. Debelle
MBM. Backman
M. Backman
LTL. Thomé
L. Thomé
William WeberWilliam Weber
William Weber
MTM. Toulemonde
M. Toulemonde
DCDidier Chaussende
Didier Chaussende
The healing effect of intense electronic energy deposition arising during swift heavy ion (SHI) irradiation is demonstrated in the case of 3C-SiC damaged by nuclear energy deposition. Experimental (ion channeling experiments) and computational (molecular dynamics simulations) studies provide consistent indications of disorder decrease after SHI irradiation. Furthermore, both methods establish that SHI-induced recrystallization takes place at amorphous-crystalline interfaces. The recovery process is unambiguously accounted for by the thermal spike phenomenon.

22 January 2023 in Materials
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HOHaiyan Ou
Haiyan Ou
XSXiaodong Shi
Xiaodong Shi
YLYaoqin Lu
Yaoqin Lu
MKManuel Kollmuß
Manuel Kollmuß
JSJohannes Steiner
Johannes Steiner
DCDidier Chaussende
Didier Chaussende
Silicon carbide (SiC) is emerging rapidly in novel photonic applications thanks to its unique photonic properties facilitated by the advances of nanotechnologies such as nanofabrication and nanofilm transfer. This review paper will start with the introduction of exceptional optical properties of silicon carbide. Then, a key structure, i.e., silicon carbide on insulator stack (SiCOI), is discussed which lays solid fundament for tight light confinement and strong light-SiC interaction in high quality factor and low volume optical cavities. As examples, microring resonator, microdisk and photonic crystal cavities are summarized in terms of quality (Q) factor, volume and polytypes. A main challenge for SiC photonic application is complementary metal-oxide-semiconductor (CMOS) compatibility and low-loss material growth. The state-of-the-art SiC with different polytypes and growth methods are reviewed and a roadmap for the loss reduction is predicted for photonic applications. Combining the fact that SiC possesses many different color centers with the SiCOI platform, SiC is also deemed to be a very competitive platform for future quantum photonic integrated circuit applications. Its perspectives and potential impacts are included at the end of this review paper.

1 January 2010 in Journal of Crystal Growth
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Journal Article
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FMFrederic Mercier
Frederic Mercier
JDJean-Marc Dedulle
Jean-Marc Dedulle
DCDidier Chaussende
Didier Chaussende
MPMichel Pons
Michel Pons

22 August 2011 in Applied Physics Letters
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Journal Article
Closed access
CCC. Coletti
C. Coletti
KEK. V. Emtsev
K. V. Emtsev
AZA. A. Zakharov
A. A. Zakharov
TOT. Ouisse
T. Ouisse
DCDidier Chaussende
Didier Chaussende
USU. Starke
U. Starke
Large scale, homogeneous quasi-free standing monolayer graphene is obtained on cubic silicon carbide, i.e., the 3C-SiC(111) surface, which represents an appealing and cost effective platform for graphene growth. The quasi-free monolayer is produced by intercalation of hydrogen under the interfacial, (63×63)R30 °-reconstructed carbon layer. After intercalation, angle resolved photoemission spectroscopy reveals sharp linear π-bands. The decoupling of graphene from the substrate is identified by x-ray photoemission spectroscopy and low energy electron diffraction. Atomic force microscopy and low energy electron microscopy demonstrate that homogeneous monolayer domains extend over areas of hundreds of square-micrometers.