Electrochemical Charging of Individual Single-Walled Carbon Nanotubes

被引:51
作者
Kalbac, Martin [1 ,3 ]
Farhat, Hootan [2 ]
Kavan, Ladislav [1 ]
Kong, Jing [3 ]
Sasaki, Ken-ichi [4 ]
Saito, Riichiro [5 ]
Dresselhaus, Mildred S. [3 ,6 ]
机构
[1] Acad Sci Czech Republic, J Heyrovsky Inst Phys Chem, CZ-18223 Prague 8, Czech Republic
[2] MIT, Dept Mat Sci & Engn, Cambridge, MA 02139 USA
[3] MIT, Dept Elect Engn & Comp Sci, Cambridge, MA 02139 USA
[4] Natl Inst Mat Sci, Tsukuba, Ibaraki 3050044, Japan
[5] Tohoku Univ, Dept Phys, Sendai, Miyagi 9808578, Japan
[6] MIT, Dept Phys, Cambridge, MA 02139 USA
关键词
single-walled carbon nanotubes; Raman spectroscopy; electrochemical gating; spectroelectrochemistry; RAMAN-SCATTERING; TRANSITION; RENORMALIZATION; DEPENDENCE; BUNDLES; ENERGY;
D O I
10.1021/nn9004318
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
The influence of the electrode potential on the electronic structure of individual single-walled carbon nanotubes is studied using Raman spectroscopy. By analyzing the radial breathing mode intensity versus electrode potential profiles in the Raman spectra at many different laser excitation energies, we show that the charging of individual carbon nanotubes causes a broadening of the resonant Raman profiles (resonance window). This effect is observed for both a semiconducting and a metallic tube. The broadening of the resonance Raman profiles already begins at potentials where the first electronic states of a particular tube are filled or depleted, The important consequence of this effect is a striking difference between the Raman intensity versus potential profiles of metallic and semiconducting tubes. While for a metallic tube the intensity of the Raman signal is attenuated at potentials which deviate slightly from 0 V, for a semiconducting tube, the Raman intensity is significantly attenuated only after the electrode potential reaches the first van Hove singularity. Furthermore, for the metallic tube, a strong asymmetry is found in the bleaching of the Raman signal with respect to positive and negative potentials, which results from the different energy bandwidth for the pi* band and the pi band.
引用
收藏
页码:2320 / 2328
页数:9
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