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Chirality dependence of coherent phonon amplitudes in single-wall carbon nanotubes

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FIG. 1. The coherent RBM phonon amplitude Q m for an (11,0) zigzag tube as a function of laser excitation energy E laser
FIG. 3. (Color online) Electron and hole components of the ETB M el-ph shown by solid and dashed lines, respectively, for (a) (11,0) and (b) (13,0) zigzag nanotubes, as a function of k
FIG. 6. (Color online) The lattice response of SWNTs with diameters in the range 0.7–1.1 nm is mapped onto the unrolled graphene lattice specifiying the tube chiralities (n,m)

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