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Beyond zone folding: effect of curvature and NT bundles Márk Géza István MTA Research Institute for Technical Physics and Materials Science Budapest http://www.nanotechnology.hu
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Outline j Introduction -- zone folding jEffect of curvature -- jellium model results jEffect of curvature -- small energy: secondary gap jEffect of curvature -- hybridization of Pi and Sigma states: shift of the bands jBundles -- low energy: secondary gap jBundles -- visible energy range: shift of the bands
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Graphene layer lattice
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Graphene 2D band structure Tigh binding first neighbor Ab-initio
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Rolling vector C h = na 1 +ma 2 C h = 3a 1 +2a 2
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Different rollings armchair zigzag general
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Nanotube bandstructure IF (n-m)/3 THEN metallic ELSE semiconductor
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Metallic tube 1D band structure
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NT density of states and tunneling spectroscopy STS J. W. Wildöer et al., Nature 391 (1998) 59
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1. effect of rolling: inequivalent neighbors Rolling a d<a Along the circumference: bond length and angle change Along the NT axis: no change
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2. effect of rolling: Pi - Sigma mixing Graphene: pure sp 2 bonds Nanotube: mixed sp 2 and sp 3 bonds
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Effect of curvature in simple jellium NT model Zone foldingCylindrical geometry
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Jellium solutions Zone folding: superposition of plane waves Cylindrical geometry: superposition of Bessel functions
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Effect of NT radius L.Tapasztó et. al., AIP Conf. Proc., 685, 439, (2003) E(r;m) functionsE(m;r) functions
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First neighbor tight binding -- inequivalent neighbors Use different 1 and 2 interaction energy for the two types of neighbors! zigzagarmchair Only armchair tubes remain true metallic because shift in k z is parallel to allowed line Zigzag: finite gap opens!
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Curvature induced gap at E F armchair points Calculated secondary gap in quasi-metallic nanotubes STS measurement 1/d 2 gap energy
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Sigma - Pi hybridization (5,0) NT m=0 eigenfunction at the Gamma point Most of the wave function concentrated outside the NT Strong component with equal sign on both sides
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Curvature effect on armchair tube Zone folding is good for armchair tubes level anticrossing
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Curvature effect: zigzag tube Pi* bands shifted down Sigma* bands shifted up
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Effect of curvature Valence bands not affected by curvature Two-fold degeneracy of Sigma* is lifted in NT Armchair Sigma* does not change Pi* band moves down Sigma* band moves up
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Nanotube bundles (or ropes) HRTEM image of NT ropeHexagonal packing of (10,10) tubes
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Effect of proximity: pseudogap Hexagonal packing of (10,10) tubes Calculated DOS
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Effect of bundles Band shifts Van-Hove singularities: - peak splitting and - decreased intensity
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