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SANS of Labeled SWNT Dispersions and Clusters

 

Introduction

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Dispersion of single wall carbon nanotubes (SWNTs) in solvents is a crucial step towards using them as components in nanomanufacturing. Common dispersion methods can produce significant contaminations of large clusters of tubes. Small angle neutron scattering (SANS) is a powerful tool in determining the effectiveness of a dispersion strategy. The clusters may either be in dynamic equilibrium with single dispersed tubes or remnants from the production process that resist dispersion.

Experimental Approach

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SWNT clusters are commonly seen by scattering. SANS of labeled tubes can determine if dynamic equilibrium exchanges tubes within the clusters,

SANS can use the “high concentration” method to extract single particle scattering from mixtures and determine if tube culsters are in dynamic equilibrium. Two samples are prepared, one in which deuterium has replaced the hydrogen of the structure. SWNTs themselves contain no hydrogen, however, free radical chemistry can be used to attach alkyl groups that supply the required hydrogen for the high contrast technique.

Scattering from concentrated mixtures have contributions from single chain correlations, P(q), and inter-chain correlations, Q(q). P(q) contains information on molecular mass, size, stiffness, etc., and Q(q) contains information on clustering, ordering, etc. For a mixture of identical SWNTs with differing contrast factors, sH and sD, dispersed in a medium with contrast factor sS, with a mole fraction of hydrogen and deuterium of xH and xD I(q) is given by:
I(q) = K MW((xD(sD - sS)2 + xH(sH - sS)2)P(q) +(xDsD + xHsH – xS)2fQ(q)
Therefore both P(q) and Q(q) can be determined from SANS of several mixtures.

 

Results

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Thermogravametric analysis (TGA) of the two SWNT materials measures composition. The mass loss in the first stage in nitrogen represents the mass fraction of butyl groups attached to the SWNT and the second stage in air burns off the SWNT. The two samples are well matched.

P(q) gives a power law of -2.5, the same as the power law of whole sample. This indicates that the structure of the scattering entity is a branched collection of SWNTs. The mixing and sonication of the clustered samples does not appear to break up the clusters, and individual tubes are not exchanged.


Tapping-mode atomic force microscopy measurements on a spin coat sample were made. Individual nanotubes have a diameter of under 1 nm. SWNT clusters were found with strong evidence of “wrapping” interaction between individual SWNTs in a fraction of the sample population.

Implications

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Dispersion of SWNT in solvents often results in formation of large clusters of individual tubes. If these clusters are remnants of ones formed in the SWNT production process, it might not be possible to easily break up these structures.
 

Production of Single SWNTs

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If the clustered species are permanent structures, it should be possible to remove them from the single SWNTs by methods such as chromatography or precipitation. Individual tubes would then be available for further manipulation and assembly.
 

Contributors:

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Barry J. Bauer, Erik K. Hobbie, Matthew L. Becker
 
 
 
 
 
 
 
 
 
 
 
 
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Processing Characterization Group
Polymers Division
Materials Science and Engineering Laboratory

 
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