Related Experiment Video
Updated: Nov 21, 2025

07:44
Resonance Raman Spectroscopy of Extreme Nanowires and Other 1D Systems
Published on: April 28, 2016
15.3K
Intense Raman D Band without Disorder in Flattened Carbon Nanotubes
Emmanuel Picheau1, Anthony Impellizzeri2, Dmitry Rybkovskiy3
1Université de Bordeaux, CNRS, Centre de Recherche Paul Pascal, UMR5031, 33600 Pessac, France.
ACS Nano
|January 14, 2021
Summary
Carbon nanotubes (CNTs) collapse into flattened structures, creating a strong Raman D band. This D band indicates structural changes, not defects, in CNTs.
Area of Science:
- Materials Science
- Nanotechnology
- Physical Chemistry
Background:
- Single- or few-walled carbon nanotubes (CNTs) can spontaneously collapse into flattened structures above a critical diameter.
- Raman spectroscopy is commonly used to assess the structural integrity and defect density of carbon-based nanomaterials.
Purpose of the Study:
- To investigate the origin of the D band in Raman spectra of collapsed CNTs.
- To determine if the D band in flattened CNTs is indicative of lattice disorder or other structural phenomena.
Main Methods:
- Recording and analyzing Raman spectra of isolated, flattened, and cylindrical CNTs.
- Performing theoretical calculations using the Placzek approximation to model the observed spectral features.
Main Results:
- The collapse of CNTs induces an intense and narrow D band in their Raman spectra.
- This D band appears despite the absence of significant lattice disorder or framework discontinuities.
- Theoretical calculations confirm that curvature changes near edge cavities activate the D band.
Conclusions:
- The D band in flattened CNTs arises from curvature changes, not lattice defects.
- The D band is not a reliable indicator of defect density in structures with graphene folds.
- This finding necessitates a re-evaluation of Raman-based conclusions regarding carbon organization in distorted materials.
Keywords:
Raman D bandRaman spectroscopycarbon nanotubescollapsed carbon nanotubesdefectsflattened carbon nanotubesMore Related Videos
Related Concept Videos
Raman Spectroscopy: Overview
981
The underlying principle of Raman spectroscopy is based on the interaction between light and matter, specifically molecules' inelastic scattering of photons. When a monochromatic beam of light, typically from a laser source, interacts with a sample, most scattered light has the same frequency as the incident light. This is known as Rayleigh scattering.
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and...
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and...
981
Raman Spectroscopy Instrumentation: Overview
675
A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
675
¹H NMR of Conformationally Flexible Molecules: Temporal Resolution
1.1K
At room temperature, the chair conformer of cyclohexane undergoes rapid ring flipping between two equivalent chair conformers at a rate of approximately 105 times per second. These two chair conformers are in equilibrium. The rapid ring flipping results in the interconversion of the axial proton to an equatorial proton and an equatorial to the axial proton. Such interconversions are too rapid and cannot be detected on the NMR timescale. Hence, the NMR spectrometer cannot distinguish between the...
1.1K

