E33 and E44 optical transitions in semiconducting single-walled carbon nanotubes:: Electron diffraction and Raman experiments

被引:39
作者
Michel, T. [1 ]
Paillet, M.
Meyer, J. C.
Popov, V. N.
Henrard, L.
Sauvajol, J.-L.
机构
[1] Univ Montpellier 2, UMR CNRS 5587, Lab Colloides Verres & Nanomat, F-34095 Montpellier 5, France
[2] Max Planck Inst Solid State Res, Stuttgart, Germany
[3] Fac Univ Notre Dame Paix, Lab Phys Solide, B-5000 Namur, Belgium
来源
PHYSICAL REVIEW B | 2007年 / 75卷 / 15期
关键词
D O I
10.1103/PhysRevB.75.155432
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
By combining, on the same freestanding single-walled carbon nanotubes, electron diffraction and Raman experiments, we were able to obtain the resonance energy of unambiguously (n,m)-identified single-walled carbon nanotubes. We focus on the analysis of the first optical transition of metallic tubes (E-11(M)) and the third and fourth transitions of semiconducting tubes (E-33(S) and E-44(S), respectively) in comparison with calculated values using a nonorthogonal tight-binding approach. For semiconducting tubes, we find that the calculated energies E-33(S) and E-44(S) have to be corrected by non-diameter-dependent (rigid) shifts of about 0.43 eV and 0.44 eV, respectively, for tubes in the 1.4-2.4-nm-diameter range. For metallic tubes in the 1.2-1.7-nm-diameter range, we show that a rigid shift (0.32 eV) of the calculated transition energy also leads to a good estimation of E-11(M). The rather large and non-diameter-dependent shifts for the third and fourth transitions in semiconducting tubes question a recent theoretical study, which relates the shifts to electron-electron correlation and exciton binding energy and suggest that the exciton binding is very small or missing for the higher transitions E-33(S) and E-44(S), contrary to the lower transitions E-11(S) and E-22(S).
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页数:5
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