Graphene nanoribbons (GNRs, also called nano-graphene ribbons or nano-graphite ribbons) are strips of graphene with width less than 100 nm. Graphene ribbons were introduced as a theoretical model by Mitsutaka Fujita and coauthors to examine the edge and nanoscale size effect in graphene.
Large quantities of width-controlled GNRs can be produced via graphite nanotomy, where applying a sharp diamond knife on graphite produces graphite nanoblocks, which can then be exfoliated to produce GNRs as shown by Vikas Berry. GNRs can also be produced by "unzipping" or axially cutting nanotubes. In one such method multi-walled carbon nanotubes were unzipped in solution by action of potassium permanganate and sulfuric acid. In another method GNRs were produced by plasma etching of nanotubes partly embedded in a polymer film. More recently, graphene nanoribbons were grown onto silicon carbide (SiC) substrates using ion implantation followed by vacuum or laser annealing. The latter technique allows any pattern to be written on SiC substrates with 5 nm precision.
GNRs were grown on the edges of three-dimensional structures etched into silicon carbide wafers. When the wafers are heated to approximately , silicon is preferentially driven off along the edges, forming nanoribbons whose structure is determined by the pattern of the three-dimensional surface. The ribbons had perfectly smooth edges, annealed by the fabrication process. Electron mobility measurements surpassing one million correspond to a sheet resistance of one ohm per square — two orders of magnitude lower than in two-dimensional graphene.
Nanoribbons narrower than 10 nm grown on a germanium wafer act like semiconductors, exhibiting a band gap. Inside a reaction chamber, using chemical vapor deposition, methane is used to deposit hydrocarbons on the wafer surface, where they react with each other to produce long, smooth-edged ribbons. The ribbons were used to create prototype transistors. At a very slow growth rate, the graphene crystals naturally grow into long nanoribbons on a specific germanium crystal facet.
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The students understand the relevant experimental and theoretical concepts of the nanoscale science. The course move from basic concepts like quantum size effects to hot fields such as spin transp
Students will learn about understanding the fundamentals and applications of emerging nanoscale devices, materials and concepts.Remark: at least 5 students should be enrolled for the course to be g
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Le graphène est un matériau bidimensionnel cristallin, forme allotropique du carbone dont l'empilement constitue le graphite. Cette définition théorique est donnée par le physicien en 1947. Par la suite, le travail de différents groupes de recherche permettra de se rendre compte que la structure du graphène tout comme ses propriétés ne sont pas uniques et dépendent de sa synthèse/extraction (détaillée dans la section Production).
thumb|Représentation d'un nanotube de carbone. (cliquer pour voir l'animation tridimensionnelle). thumb|Un nanotube de carbone monofeuillet. thumb|Extrémité d'un nanotube, vue au microscope électronique. Les nanotubes de carbone (en anglais, carbon nanotube ou CNT) sont une forme allotropique du carbone appartenant à la famille des fullerènes. Ils sont composés d'un ou plusieurs feuillets d'atomes de carbone enroulés sur eux-mêmes formant un tube. Le tube peut être fermé ou non à ses extrémités par une demi-sphère.
Explore la spectroscopie électronique, les propriétés du graphène et les effets de polarisation de spin, offrant un aperçu de l'optimisation des propriétés des matériaux et des applications potentielles.
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2024
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