Structural and optical properties of size controlled Si nanocrystals in Si3N4 matrix: The nature of photoluminescence peak shift
Creators
- 1. Faculty of Engineering, IMTEK, Albert-Ludwigs-University Freiburg, Georges-Köhler-Allee 103, 79110 Freiburg (Germany)
- 2. Optics and Photonics, School of Information and Communication Technology, Royal Institute of Technology (KTH), Electrum 229, Kista SE-16440 (Sweden)
- 3. Department of Electronic and Electrical Engineering, Trinity College Dublin, Dublin 2 (Ireland)
- 4. Institute for Applied Materials (IAM) and Karlsruhe Nano Micro Facility, Karlsruhe Institute of Technology, Hermann-von-Helmholtz-Platz 1, 76344 Eggenstein-Leopoldshafen (Germany)
- 5. MATIS IMM-CNR, Universita' di Catania, Via S. Sofia 64, I-95123 Catania (Italy)
- 6. Fraunhofer-Institut für Solare Energiesysteme ISE Heidenhofstr. 2, 79110 Freiburg (Germany)
- 7. MIND-IN2UB, Departament d'Electrònica, Universitat de Barcelona, C/Martí i Franquès, 1, 08028 Barcelona (Spain)
- 8. CCiT, Scientific and Technical Centers, Universitat de Barcelona, C/Lluís Solé i Sabaris 1, 08028 Barcelona (Spain)
Description
Superlattices of Si3N4 and Si-rich silicon nitride thin layers with varying thickness were prepared by plasma enhanced chemical vapor deposition. After high temperature annealing, Si nanocrystals were formed in the former Si-rich nitride layers. The control of the Si quantum dots size via the SiNx layer thickness was confirmed by transmission electron microscopy. The size of the nanocrystals was well in agreement with the former thickness of the respective Si-rich silicon nitride layers. In addition X-ray diffraction evidenced that the Si quantum dots are crystalline whereas the Si3N4 matrix remains amorphous even after annealing at 1200 °C. Despite the proven Si nanocrystals formation with controlled sizes, the photoluminescence was 2 orders of magnitude weaker than for Si nanocrystals in SiO2 matrix. Also, a systematic peak shift was not found. The SiNx/Si3N4 superlattices showed photoluminescence peak positions in the range of 540–660 nm (2.3–1.9 eV), thus quite similar to the bulk Si3N4 film having peak position at 577 nm (2.15 eV). These rather weak shifts and scattering around the position observed for stoichiometric Si3N4 are not in agreement with quantum confinement theory. Therefore theoretical calculations coupled with the experimental results of different barrier thicknesses were performed. As a result the commonly observed photoluminescence red shift, which was previously often attributed to quantum-confinement effect for silicon nanocrystals, was well described by the interference effect of Si3N4 surrounding matrix luminescence
Additional details
Identifiers
- DOI
- 10.1063/1.4830026;
Publishing Information
- Journal Title
- Journal of Applied Physics
- Journal Volume
- 114
- Journal Issue
- 18
- Journal Page Range
- p. 184311-184311.9
- ISSN
- 0021-8979
- CODEN
- JAPIAU
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 45080508
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; S77: NANOSCIENCE AND NANOTECHNOLOGY;
- Descriptors DEI
- ANNEALING; CHEMICAL VAPOR DEPOSITION; DIFFUSION BARRIERS; LAYERS; OPTICAL PROPERTIES; PHOTOLUMINESCENCE; PLASMA; QUANTUM DOTS; RED SHIFT; SILICA; SILICON; SILICON NITRIDES; SILICON OXIDES; SUPERLATTICES; THIN FILMS; TRANSMISSION ELECTRON MICROSCOPY; VENTILATION BARRIERS; X-RAY DIFFRACTION
- Descriptors DEC
- CHALCOGENIDES; CHEMICAL COATING; COHERENT SCATTERING; DEPOSITION; DIFFRACTION; ELECTRON MICROSCOPY; ELEMENTS; EMISSION; ENGINEERED SAFETY SYSTEMS; FILMS; HEAT TREATMENTS; LUMINESCENCE; MICROSCOPY; MINERALS; NANOSTRUCTURES; NITRIDES; NITROGEN COMPOUNDS; OXIDE MINERALS; OXIDES; OXYGEN COMPOUNDS; PHOTON EMISSION; PHYSICAL PROPERTIES; PNICTIDES; SCATTERING; SEMIMETALS; SILICON COMPOUNDS; SURFACE COATING
Optional Information
- Notes
- (c) 2013 AIP Publishing LLC