2000
DOI: 10.1016/s0379-6779(00)00318-0
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Doping mechanism in single-wall carbon nanotubes studied by optical absorption

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Cited by 59 publications
(63 citation statements)
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“…However, if the applied potential moves to 2.45 V, the dopinggenerated band shifts to 1.3 eV because lower v s n states are activated. The final peak position is identical to that reported upon Cs-doping, [17,27] if we assume symmetric electronic structure. In other words, Br 2 is an insufficiently strong oxidant for depletion of deep singularities in the valence band (v s n ), but electrochemistry in ionic liquids allows such a strong oxidation easily.…”
Section: Cyclic Voltammetrysupporting
confidence: 80%
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“…However, if the applied potential moves to 2.45 V, the dopinggenerated band shifts to 1.3 eV because lower v s n states are activated. The final peak position is identical to that reported upon Cs-doping, [17,27] if we assume symmetric electronic structure. In other words, Br 2 is an insufficiently strong oxidant for depletion of deep singularities in the valence band (v s n ), but electrochemistry in ionic liquids allows such a strong oxidation easily.…”
Section: Cyclic Voltammetrysupporting
confidence: 80%
“…The exciting photons (energies 2.41 eV or 2.54 eV) resonate with the transition (v s 3 3c s 3 ) in tubes of diameters 1.2 ± 1.5 nm. [17,29,30] The overall intensities of the RBM and TM modes decrease as a result of both cathodic and anodic charging in ionic liquid (Figure 4 and (5)), which matches the behavior in aqueous [20,39,40] and aprotic [8,12,21] electrolyte solutions. By comparing Figure 4 with Figure 6 and Figure 5 with Figure 7, the tube-related modes in peapods show a similar response to electrochemical charging as those of empty tubes.…”
Section: Raman Spectroscopysupporting
confidence: 70%
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