Ion-Beam-Induced Amorphization and Epitaxial Crystallization of Silicon
Identifieur interne : 008535 ( Main/Merge ); précédent : 008534; suivant : 008536Ion-Beam-Induced Amorphization and Epitaxial Crystallization of Silicon
Auteurs : J. S. Williams [Australie] ; G. De M. Azevedo [Australie] ; H. Bernas [France] ; F. Fortuna [France]Source :
- Topics in Applied Physics [ 0303-4216 ] ; 2010.
Descripteurs français
- Wicri :
- topic : Simulation.
English descriptors
- KwdEn :
- Activation energy, Amorphization, Amorphous, Amorphous layer, Amorphous layers, Amorphous phase, Amorphous region, Amorphous silicon, Annealing, Appl, Atomic displacements, Bernas, Cascade, Cascade density, Computer simulations, Crystalline, Crystalline region, Crystalline side, Crystalline silicon, Crystallization, Defect, Defect accumulation, Defect annihilation, Defect clusters, Defect generation, Defect interactions, Deposition, Dynamic annealing, Elliman, Epitaxial, Epitaxial crystallization, Epitaxial growth, Exponent, Free energy, Front interface, Growth rate, Growth speed, Ibiec, Ibiec growth, Ibiec growth rate, Ibiec observations, Ibiec process, Ibiec rate, Ibiec rates, Ibiec regrowth, Implant, Implantation, Implantation temperature, Instrum, Interface, Interface evolution, Interface motion, Interface roughness, Interfacial energy, Interfacial growth, Irradiation conditions, Irradiation temperature, Kink, Kinomura, Lattice, Layer, Lett, Linnros, Major role, Marlowe calculations, Mater, Methods phys, Mobile defects, Monte carlo simulations, Nucl, Nucleation, Phys, Point defects, Precipitation, Preferential amorphization, Priolo, Proc, Random irradiations, Regrowth, Rimini, Room temperature, Roughness, Silicon, Simulation, Solid line, Speg, Such processes, Surface growth, Surface relaxation, Symp, Temperature dependence, Xtem, Xtem images.
- Teeft :
- Activation energy, Amorphization, Amorphous, Amorphous layer, Amorphous layers, Amorphous phase, Amorphous region, Amorphous silicon, Annealing, Appl, Atomic displacements, Bernas, Cascade, Cascade density, Computer simulations, Crystalline, Crystalline region, Crystalline side, Crystalline silicon, Crystallization, Defect, Defect accumulation, Defect annihilation, Defect clusters, Defect generation, Defect interactions, Deposition, Dynamic annealing, Elliman, Epitaxial, Epitaxial crystallization, Epitaxial growth, Exponent, Free energy, Front interface, Growth rate, Growth speed, Ibiec, Ibiec growth, Ibiec growth rate, Ibiec observations, Ibiec process, Ibiec rate, Ibiec rates, Ibiec regrowth, Implant, Implantation, Implantation temperature, Instrum, Interface, Interface evolution, Interface motion, Interface roughness, Interfacial energy, Interfacial growth, Irradiation conditions, Irradiation temperature, Kink, Kinomura, Lattice, Layer, Lett, Linnros, Major role, Marlowe calculations, Mater, Methods phys, Mobile defects, Monte carlo simulations, Nucl, Nucleation, Phys, Point defects, Precipitation, Preferential amorphization, Priolo, Proc, Random irradiations, Regrowth, Rimini, Room temperature, Roughness, Silicon, Simulation, Solid line, Speg, Such processes, Surface growth, Surface relaxation, Symp, Temperature dependence, Xtem, Xtem images.
Abstract
Abstract: Ion-induced collisions produce athermal atomic movements at and around the surface or interface, inducing step formation and modifying growth conditions. The latter may be controlled by varying the temperature and ion-beam characteristics, guiding the system between nonequilibrium and quasiequilibrium states. Silicon is an ideal material to observe and understand such processes. For ion irradiation at or below room temperature, damage due to collision cascades leads to Si amorphization. At temperatures where defects are mobile and interact, irradiation can lead to layer-by-layer amorphization, whereas at higher temperatures irradiation can lead to the recrystallization of previously amorphized layers. This chapter focuses on the role of ion beams in the interface evolution. We first give an overview of ion beam-induced epitaxial crystallization (IBIEC) and ion-beam-induced amorphization as observed in silicon and identify unresolved issues. Similarities and differences with more familiar surface thermal growth processes are emphasized. Theories and computer simulations developed for surface relaxation help us to quantify several important aspects of IBIEC. Recent experiments provide insight into the influence of ion-induced defect interactions on IBIEC, and are also partly interpreted via computer simulations. The case of phase transformations and precipitation at interfaces is also considered.
Url:
DOI: 10.1007/978-3-540-88789-8_4
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Activation energy</term>
<term>Amorphization</term>
<term>Amorphous</term>
<term>Amorphous layer</term>
<term>Amorphous layers</term>
<term>Amorphous phase</term>
<term>Amorphous region</term>
<term>Amorphous silicon</term>
<term>Annealing</term>
<term>Appl</term>
<term>Atomic displacements</term>
<term>Bernas</term>
<term>Cascade</term>
<term>Cascade density</term>
<term>Computer simulations</term>
<term>Crystalline</term>
<term>Crystalline region</term>
<term>Crystalline side</term>
<term>Crystalline silicon</term>
<term>Crystallization</term>
<term>Defect</term>
<term>Defect accumulation</term>
<term>Defect annihilation</term>
<term>Defect clusters</term>
<term>Defect generation</term>
<term>Defect interactions</term>
<term>Deposition</term>
<term>Dynamic annealing</term>
<term>Elliman</term>
<term>Epitaxial</term>
<term>Epitaxial crystallization</term>
<term>Epitaxial growth</term>
<term>Exponent</term>
<term>Free energy</term>
<term>Front interface</term>
<term>Growth rate</term>
<term>Growth speed</term>
<term>Ibiec</term>
<term>Ibiec growth</term>
<term>Ibiec growth rate</term>
<term>Ibiec observations</term>
<term>Ibiec process</term>
<term>Ibiec rate</term>
<term>Ibiec rates</term>
<term>Ibiec regrowth</term>
<term>Implant</term>
<term>Implantation</term>
<term>Implantation temperature</term>
<term>Instrum</term>
<term>Interface</term>
<term>Interface evolution</term>
<term>Interface motion</term>
<term>Interface roughness</term>
<term>Interfacial energy</term>
<term>Interfacial growth</term>
<term>Irradiation conditions</term>
<term>Irradiation temperature</term>
<term>Kink</term>
<term>Kinomura</term>
<term>Lattice</term>
<term>Layer</term>
<term>Lett</term>
<term>Linnros</term>
<term>Major role</term>
<term>Marlowe calculations</term>
<term>Mater</term>
<term>Methods phys</term>
<term>Mobile defects</term>
<term>Monte carlo simulations</term>
<term>Nucl</term>
<term>Nucleation</term>
<term>Phys</term>
<term>Point defects</term>
<term>Precipitation</term>
<term>Preferential amorphization</term>
<term>Priolo</term>
<term>Proc</term>
<term>Random irradiations</term>
<term>Regrowth</term>
<term>Rimini</term>
<term>Room temperature</term>
<term>Roughness</term>
<term>Silicon</term>
<term>Simulation</term>
<term>Solid line</term>
<term>Speg</term>
<term>Such processes</term>
<term>Surface growth</term>
<term>Surface relaxation</term>
<term>Symp</term>
<term>Temperature dependence</term>
<term>Xtem</term>
<term>Xtem images</term>
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<keywords scheme="Teeft" xml:lang="en"><term>Activation energy</term>
<term>Amorphization</term>
<term>Amorphous</term>
<term>Amorphous layer</term>
<term>Amorphous layers</term>
<term>Amorphous phase</term>
<term>Amorphous region</term>
<term>Amorphous silicon</term>
<term>Annealing</term>
<term>Appl</term>
<term>Atomic displacements</term>
<term>Bernas</term>
<term>Cascade</term>
<term>Cascade density</term>
<term>Computer simulations</term>
<term>Crystalline</term>
<term>Crystalline region</term>
<term>Crystalline side</term>
<term>Crystalline silicon</term>
<term>Crystallization</term>
<term>Defect</term>
<term>Defect accumulation</term>
<term>Defect annihilation</term>
<term>Defect clusters</term>
<term>Defect generation</term>
<term>Defect interactions</term>
<term>Deposition</term>
<term>Dynamic annealing</term>
<term>Elliman</term>
<term>Epitaxial</term>
<term>Epitaxial crystallization</term>
<term>Epitaxial growth</term>
<term>Exponent</term>
<term>Free energy</term>
<term>Front interface</term>
<term>Growth rate</term>
<term>Growth speed</term>
<term>Ibiec</term>
<term>Ibiec growth</term>
<term>Ibiec growth rate</term>
<term>Ibiec observations</term>
<term>Ibiec process</term>
<term>Ibiec rate</term>
<term>Ibiec rates</term>
<term>Ibiec regrowth</term>
<term>Implant</term>
<term>Implantation</term>
<term>Implantation temperature</term>
<term>Instrum</term>
<term>Interface</term>
<term>Interface evolution</term>
<term>Interface motion</term>
<term>Interface roughness</term>
<term>Interfacial energy</term>
<term>Interfacial growth</term>
<term>Irradiation conditions</term>
<term>Irradiation temperature</term>
<term>Kink</term>
<term>Kinomura</term>
<term>Lattice</term>
<term>Layer</term>
<term>Lett</term>
<term>Linnros</term>
<term>Major role</term>
<term>Marlowe calculations</term>
<term>Mater</term>
<term>Methods phys</term>
<term>Mobile defects</term>
<term>Monte carlo simulations</term>
<term>Nucl</term>
<term>Nucleation</term>
<term>Phys</term>
<term>Point defects</term>
<term>Precipitation</term>
<term>Preferential amorphization</term>
<term>Priolo</term>
<term>Proc</term>
<term>Random irradiations</term>
<term>Regrowth</term>
<term>Rimini</term>
<term>Room temperature</term>
<term>Roughness</term>
<term>Silicon</term>
<term>Simulation</term>
<term>Solid line</term>
<term>Speg</term>
<term>Such processes</term>
<term>Surface growth</term>
<term>Surface relaxation</term>
<term>Symp</term>
<term>Temperature dependence</term>
<term>Xtem</term>
<term>Xtem images</term>
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<front><div type="abstract" xml:lang="en">Abstract: Ion-induced collisions produce athermal atomic movements at and around the surface or interface, inducing step formation and modifying growth conditions. The latter may be controlled by varying the temperature and ion-beam characteristics, guiding the system between nonequilibrium and quasiequilibrium states. Silicon is an ideal material to observe and understand such processes. For ion irradiation at or below room temperature, damage due to collision cascades leads to Si amorphization. At temperatures where defects are mobile and interact, irradiation can lead to layer-by-layer amorphization, whereas at higher temperatures irradiation can lead to the recrystallization of previously amorphized layers. This chapter focuses on the role of ion beams in the interface evolution. We first give an overview of ion beam-induced epitaxial crystallization (IBIEC) and ion-beam-induced amorphization as observed in silicon and identify unresolved issues. Similarities and differences with more familiar surface thermal growth processes are emphasized. Theories and computer simulations developed for surface relaxation help us to quantify several important aspects of IBIEC. Recent experiments provide insight into the influence of ion-induced defect interactions on IBIEC, and are also partly interpreted via computer simulations. The case of phase transformations and precipitation at interfaces is also considered.</div>
</front>
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