Resonance Raman and infrared spectroscopy of carbon nanotubes

J. Kastner; T. Pichler; H. Kuzmany; S. Curran; W. Blau; D. N. Weldon; M. Delamesiere; S. Draper; H. Zandbergen

doi:10.1016/0009-2614(94)87015-2

Resonance Raman and infrared spectroscopy of carbon nanotubes

J. Kastner, T. Pichler, H. Kuzmany, S. Curran, W. Blau, D. N. Weldon, M. Delamesiere, S. Draper, H. Zandbergen

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Abstract

We present a comparative analysis of the vibrational and structural properties of carbon nanotubes. The first-order Raman spectrum exhibits two lines at 1582 cm^-1 and at 1350 cm^-1. The observed ratio of the integrated intensity of these lines was found to be different as compared to polycrystalline graphite. The position and intensity of the line around 1350 cm^-1 strongly depend on the energy of the exciting laser line. This dispersion effect is again different from the dispersion in nanocrystalline graphite. It is discussed in terms of a photoselective resonance process. Transmission infrared spectra of the nanotubes show one broad and asymmetric line at 1575 cm^-1 and a weaker line at 868 cm^-1.

Original language	English
Pages (from-to)	53-58
Number of pages	6
Journal	Chemical Physics Letters
Volume	221
Issue number	1-2
DOIs	https://doi.org/10.1016/0009-2614(94)87015-2
Publication status	Published - 15 Apr 1994
Externally published	Yes

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title = "Resonance Raman and infrared spectroscopy of carbon nanotubes",

abstract = "We present a comparative analysis of the vibrational and structural properties of carbon nanotubes. The first-order Raman spectrum exhibits two lines at 1582 cm-1 and at 1350 cm-1. The observed ratio of the integrated intensity of these lines was found to be different as compared to polycrystalline graphite. The position and intensity of the line around 1350 cm-1 strongly depend on the energy of the exciting laser line. This dispersion effect is again different from the dispersion in nanocrystalline graphite. It is discussed in terms of a photoselective resonance process. Transmission infrared spectra of the nanotubes show one broad and asymmetric line at 1575 cm-1 and a weaker line at 868 cm-1.",

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T1 - Resonance Raman and infrared spectroscopy of carbon nanotubes

AU - Kastner, J.

AU - Pichler, T.

AU - Kuzmany, H.

AU - Curran, S.

AU - Blau, W.

AU - Weldon, D. N.

AU - Delamesiere, M.

AU - Draper, S.

AU - Zandbergen, H.

PY - 1994/4/15

Y1 - 1994/4/15

N2 - We present a comparative analysis of the vibrational and structural properties of carbon nanotubes. The first-order Raman spectrum exhibits two lines at 1582 cm-1 and at 1350 cm-1. The observed ratio of the integrated intensity of these lines was found to be different as compared to polycrystalline graphite. The position and intensity of the line around 1350 cm-1 strongly depend on the energy of the exciting laser line. This dispersion effect is again different from the dispersion in nanocrystalline graphite. It is discussed in terms of a photoselective resonance process. Transmission infrared spectra of the nanotubes show one broad and asymmetric line at 1575 cm-1 and a weaker line at 868 cm-1.

AB - We present a comparative analysis of the vibrational and structural properties of carbon nanotubes. The first-order Raman spectrum exhibits two lines at 1582 cm-1 and at 1350 cm-1. The observed ratio of the integrated intensity of these lines was found to be different as compared to polycrystalline graphite. The position and intensity of the line around 1350 cm-1 strongly depend on the energy of the exciting laser line. This dispersion effect is again different from the dispersion in nanocrystalline graphite. It is discussed in terms of a photoselective resonance process. Transmission infrared spectra of the nanotubes show one broad and asymmetric line at 1575 cm-1 and a weaker line at 868 cm-1.

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DO - 10.1016/0009-2614(94)87015-2

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Resonance Raman and infrared spectroscopy of carbon nanotubes

Abstract

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