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5h symmetry.
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The Coulson model is equivalent to assuming that the wave functions have nodes on the missing sections beyond the tube ends. In applying the Coulson model to all of the states in Figure 1, we are generalizing to the usual envelope function model and applying this nodal condition. For odd N, J values up to (N + 1)/2 are included. We also neglect mixing between states of the same symmetry coming from different bands.
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When curvature is not considered, the Fermi momentum is exactly 2/3 of the zone boundary.
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In an analogous situation, η is called the "quasiparticle band gap" in the semiconductor nanocrystal literature when the HOMO-LUMO gap dominates.
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