Upload
abrahamchavez
View
216
Download
0
Embed Size (px)
Citation preview
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
1/8
ISSN:1369 7021 Elsevier Ltd 2007JAN-FEB 2007 | VOLUME 10 | NUMBER 1-228
Carbon nanotubes becoming clean
Carbon nanotubes (CNTs) are now well into their teenage years. Early
on, theoretical predictions and experimental data showed that CNTs
possess chemical and mechanical properties that exceed those of manyother materials. This has triggered intense research into CNTs. A variety
of production methods for CNTs have been developed; chemical
modification, functionalization, filling, and doping have been achieved; and
manipulation, separation, and characterization of individual CNTs is now
possible. Today, products containing CNTs range from tennis rackets
and golf clubs to vehicle fenders, X-ray tubes, and Li ion batteries.
Breakthroughs for CNT-based technologies are anticipated in the areas
of nanoelectronics, biotechnology, and materials science. In this article,
I review the current situation in CNT production and highlight the
importance of clean CNT material for the success of future applications.
Nicole Grobert
Department of Materials, University of Oxford, Parks Road, Oxford, OX1 3PH, UK
E-mail: [email protected]
Carbon fibers and filaments have been studied for over 100 years.
Hughes and Chambers1, and Schtzenberger and Schtzenberger2
reported the growth of filamentous carbon in 1889 and 1890,
respectively. In the early 1950s, Radushkevich and Lukyanovich3
published a report on hollow carbon fibers (Fig. 1). Since then,
the demand by the space and aerospace industry for stronger,
lightweight materials with improved mechanical properties has led
to substantial progress in the production and characterization of
carbon filaments and hollow carbon fibers.
History of carbon nanotubesEarly on, it was realized that generating highly crystalline carbon fibers
resistant to crack propagation would require further development of
growth methods such as chemical vapor deposition. In the 1970s, Endo
et al.4 showed a viewgraph of what is now called a single- or double-
walled carbon nanotube (SWNT or DWNT) (Fig. 2). At that time,
although electron microscopes were powerful enough to study the
structure of the carbon filaments in detail, the images did not reveal
the number of walls clearly. For example, it cannot be determined
mailto:[email protected]:[email protected]8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
2/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-2
whether the nanotube inFig. 2 consists of one or two concentric
graphene cylinders (Fig. 3)4,5. The carbon fiber community then was
familiar with filament-like structures and did not pay further attention
to smaller-scale objects like the CNTs observed by Endo et al.4. Instead,
research focused on generating carbon fibers from polymer-based
precursors using rayon, polyacrylonitrile (PAN), or mesophase pitch.
Graphitic nanofibers were also encountered by the catalysis
community and steel industry. Here, carbon nanofibers were, and still
are, considered unwanted byproducts causing poisoning6 of metal
catalyst particles or damage to reactor walls in furnaces7. This process
is also known as metal dusting or corrosion (Fig. 4)8-10.
Yet the paper entitled Helical microtubules of graphitic carbon
published by Iijima in 199111 caused an unprecedented change in
carbon science. Iijima was fascinated by the Krtschmer-Huffman paper
on the lab-scale production of C6012. He examined soot produced
by the Krtschmer-Huffman method provided by Ando12,13 using a
high-resolution transmission electron microscope (HRTEM). In 1990,
Iijima presented images of carbon nanotubes (Fig. 5) at a meeting
in Richmond, Virginia and one month later he published his paper in
Nature11. A combination of factors was responsible for the tremendous
impact of Iijimas paper and for the attention that these graphitic
nanofibers continue to attract today14. 15 years later, the number of
publications related to CNTs is still increasing exponentially.
Motivation carbon nanotube propertiesIdeal CNTs may be described as nanoscale graphene cylinders that are
closed at each end by half a fullerene. Structures comprising only one
cylinder are termed SWNTs, whereas multiwalled nanotubes (MWNTs)
contain two or more concentric graphene cylinders. Ideal SWNTs are
classified according to three possible crystallographic configurations,
zigzag, armchair, and chiral, depending on how the graphene sheet
is rolled up. In the zigzag conformation, two opposite C-C bonds of
each hexagon are parallel to the tube axis, whereas in the armchair
conformation the C-C bonds are perpendicular to the axis. In all other
arrangements, the opposite C-C bonds lie at an angle to the tube axis,
resulting in a so-called helical nanotube that is chiral (Fig. 6).
Fig. 1 Low-resolution transmission electron micrograph depicting three hollowcarbon fibers at MAG 20 000. These fibers were first reported by Radushkevichand Lukyanovich in 1950. (Adapted and reprinted with permission from 3.)
Fig. 2 First viewgraph of what today is called SWNT or DWNT. Based on thisimage, it is difficult to determine the exact number of walls. (Adapted andreprinted with permission from4. 1976 Elsevier.)
Fig. 3 Simulated images of a DWNT in a SWNT bundle and a SWNT in aDWNT bundle. To avoid misinterpretation of such complicated transmissionelectron micrograph images, the authors suggest analyzing the cross sectionof the nanotubes and bundles. If possible, TEM images should be combinedwith image simulations and other characterization methods, e.g. Raman
spectroscopy. (Adapted and reprinted with permission from5
. 2006 Elsevier.)
Carbon nanotubes becoming clean REVIEW
Fig. 4 Typical scanning electron micrograph of the carbon filaments oftenobserved during metal dusting processes. (Scale bar = 2 m.)
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
3/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-230
CNTs may exhibit extraordinary aspect ratios. SWNTs are found to
grow up to several centimeters long15, i.e. 109 times their diameter.MWNTs exhibit lengths of up to a centimeter16and have diameters
from 5-100 nm. CNT properties are strongly dependent on their
structure, e.g. for typical diameters, all armchair SWNTs and one-third
of all zigzag nanotubes are metallic, the rest are semiconducting17.
Extraordinary mechanical properties of SWNTs were predicted
shortly after their discovery18. Doping of CNTs can be used to tune
their electronic response19. Several accounts have shown that CNTs can
act as field-effect transistors20 or that vertically aligned CNTs are ideal
candidates for low-resistance interconnects21,22 (Figs. 7aand b).
These properties make CNTs attractive for applications in
nanoelectronics20 and quantum computing23, as gas sensors24-26, or
fillers in polymer27, ceramic28,29, or metal30 composites31. Today,
numerous spin-off companies offer CNTs at competitive prices, and
more and more products containing CNTs are becoming available.
However, no currently available CNT-based application makes use
of the properties of individual nanotubes. To date, all commercial CNT-
based applications rely on the bulk properties of CNT ensembles. The
much anticipated breakthrough ofindividual CNTs, e.g. in electronic
devices, has yet to be achieved. One of the key limiting factors is the
unavailability of clean materials. As discussed in the following sections,
current growth methods are insufficient for the controlled production
of CNTs with uniform structure and uniform properties.
Properties of individual carbon nanotubesThe data reported for mechanical and electrical properties of CNTs
vary significantly.Table 1 shows the variation in experimentally
determined values of the Youngs modulus and tensile strength. Often,
measurements have to be carried out on several tubes until expected
results are found and confirmed, because of the variation in structure
exhibited by different nanotubes. This is disconcerting because
applications require uniform properties, yet it is self-evident because
current synthesis methods cannot yet generate monochiral nanotubes,
i.e. nanotubes of the same atomic structure and hence properties. The
inconsistency of results can be understood as follows. First, nanotubes
contained in a typical sample differ in length, diameter, chirality, and
number of walls, or, more generally, in their atomic structure. Second,
nanotubes produced via different methods contain different levels of
defects and byproducts. While some labs specialize in the production
of CNTs, others carry out physical measurements, such as spectroscopy
and microscopy, on samples obtained through collaborations or from
Fig. 5 Iijimas TEM micrographs of three MWNTs consisting of three, five, andseven concentric graphene shells. (Adapted and reprinted with permissionfrom11. 1991 Nature Publishing Group.)
Fig. 6 Models of three atomically perfect SWNT structures.
REVIEW Carbon nanotubes becoming clean
(b)(a) (c)
Table 1 Variation of Youngs modulus and tensile strength found for different carbon nanotubes.
Author Youngs modulus[TPa]
Tensile strength[TPa]
Nanotube type Method
Treacy et al.102 1.8 MWNTARC thermal vibrations (TEM)
Krishnan et al.103 1.25 SWNTLSR thermal vibrations (TEM)
Wong et al.104 1.28 MWNTARC AFM
Salvetat et al.105 0.81 MWNTARC AFM
Salvetat et al.106 0.01-0.05 MWNTCVD AFM
Yu et al.107 0.27-0.95 0.01-0.06 MWNTARC AFM (dual cantilevers)
Demczyk et al.108 0.8 0.15 MWNTARC TEM (tension)
Bacon109 0.8 Carbon whiskers
Edie et al.110 0.2-0.9 0.002-0.007 Carbon fibers
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
4/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-2
commercial suppliers. Therefore, a detailed characterization of the CNT
material is not available, because companies and labs specializing in
CNT synthesis often do not have access to or cannot afford detailed
and time consuming structural characterization of each CNT batch.
Often, only the first samples produced using a new process are studied
in detail. Subsequent batches are assumed to exhibit similar features.
Unfortunately, this approach is unsuitable for CNT evaluation because
small fluctuations in synthesis conditions can change the structure of
CNTs dramatically.
Carbon nanotube synthesisThe principle of CNT production is simple. All known production
techniques involve a carbon feedstock, a metal catalyst, and heat. All
methods for producing SWNTs require a metal catalyst, while in the
production of MWNTs, carbon arc discharge is the one exception that
does not require any metal catalyst. Several books and reviews13,32-35
describe CNT production methods, hence I will focus on the properties
of MWNTs and SWNTs obtained through different methods.
Carbon arc discharge
In 1992, Ebbesen and Ajayan36 showed that MWNTs can be produced
in a carbon arc discharge (Figs.8a, 8b, 9a, and 9b). The carbon arc
discharge uses two graphite electrodes through which a direct current
is passed in an inert He atmosphere. The anode is consumed and a
cigar-like deposit forms on the cathode. The outer shell of this deposit
is gray and hard with a black soft inner core that contains MWNTs,
polyhedral particles, and amorphous carbon36. SWNTs may also be
obtained but require mixed metal catalysts, such as Fe:Co, Ni:Y37, that
are inserted into the anode. After arcing, SWNTs are found distributed
in the chamber as a fluffy web-like material37. Ando13 showed that the
arc evaporation of a graphite rod with a pure Fe catalyst in conjunction
with a hydrogen and inert gas mixture may be used for growing
macroscopic SWNT nets of up to 20-30 cm in length. Replacing He by
H2 results in MWNTs with a very thin innermost tube of
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
5/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-232
as ropes or bundles consisting of several individual SWNTs. Byproducts
such as amorphous carbon or encapsulated metal catalyst particles are
also present. The laser-ablation technique favors the growth of SWNTs;
MWNTs are usually not generated with this method. The quality,
length, diameter, and chirality distribution of the material are believed
to be comparable with those of SWNTs grown by arc discharge.
Chemical vapor deposition (CVD)
The catalyzed decomposition of hydrocarbons has been known to
generate carbon fibers since filamentous carbon was produced by
passing cyanogen over red-hot porcelain in 18902. In the 1980s, Endo48
developed the floating catalyst reactor using catalyst particles 10 nm
in diameter. This method is a precursor to the aerosol-based CNT
production widely used today49-55, where pyrolysis of hydrocarbons
in the presence of a transition metal catalyst (Fe, Ni, Co, etc .)
generates MWNTs and SWNTs. MWNTs are mainly produced at lower
temperatures (300-800C) in an inert gas atmosphere, whereas SWNTs
require higher temperatures (600-1150C)45,56-58 and a mixture of H2
and an inert gas such as Ar. DWNT generation using CVD techniques
involves a more complicated catalyst preparation procedure. DWNT
samples generally also contain SWNTs and triple-walled CNTs59.
The decomposition of hydrocarbons is aided by a plasma in plasma-
enhanced CVD (PECVD) or plasma-assisted CVD (PACVD). Park et
al.60 used a combination of CVD and PECVD to create CNTs from an
acetylene and H2 gas mixture on stainless steel plates. CVD and PECVD
are commonly used to grow aligned MWNTs (Figs.8c and d), and
SWNTs on various substrates including Ni61, Si62, SiO249,53,54,63,64,
Cu/Ti/Si(100)65, stainless steel60,66, glass67, etc. The structure of
MWNTs produced by CVD, in particular, differs significantly from
MWNTs generated by arc discharge (MWNTARC). For example, CVD-
grown MWNTs (MWNTCVD) are usually less crystalline and exhibitmany more defects than MWNTARC. Therefore, MWNTCVD are less
straight than MWNTARC(Figs. 9c and d). In some instances, depending
on the catalyst, spiral growth can be observed (Fig. 10) 64,68-70.
CVD is probably the most versatile production method for
CNTs, especially for generating doped CNTs, e.g. with B, N, or
both19,54,63,64,68,71-76. MWNTCVD can reach a centimeter in length and
usually possess larger diameters of up to 100 nm. The number of walls
in MWNTCVD can vary from three to >100. MWNTCVD usually grow
perpendicular to the substrate; therefore their length is relatively easy
to measure (Figs. 8c and 11). The CNT and carbon-fiber communities
are still debating at what diameter CNTs should still be called CNTs
and from what diameter the structures are carbon nanofibers.
Electrolysis
Electrolysis is a less common method for CNT production. To date,
it is the only condensed phase method for generating CNTs, and was
developed by Hsu et al. in 199577,78. MWNTs are formed when a
current is passed through two graphite electrodes immersed in molten
REVIEW Carbon nanotubes becoming clean
Fig. 9 TEM images reveal the structural differences of MWNTs produced via CVDtechniques and by arc discharge. (a) TEM image of raw MWNTARCrevealing the
presence of polyhedral carbon particles. (b) TEM image of purified MWNTARC.(c) TEM images of nanotubes generated by pyrolysing 2-amino-4,6-dichloro-s-triazine over laser-etched Co substrates. (d) MWNTCVD exhibiting metalparticles (~40 nm OD) at their ends; inset showing a close-up of the particlecontaining nanotube tips. (Parts (a),(b) adapted and reprinted with permissionfrom101. Parts (c),(d) adapted and reprinted with permission from 64. 1999and 2000 Springer.)
Fig. 10 SEM image of carbon nanocoils generated by pyrolysis of melamine overCo-oxide substrates.
Fig. 11 SEM image of a bundle of MWNTCVD with a human hair for comparison.Here, the length of the MWNTCVD is roughly the same as the diameter of thehuman hair, 80 m.
(b)
(a) (c)
(d)
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
6/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-2
ionic salts, such as LiCl at 600C. After electrolysis, the carbonaceous
material is extracted by dissolving the ionic salt in distilled water and
separating the dispersion by filtration. The material produced contains
MWNTs, carbon-encapsulated metal particles from the salt ions,amorphous carbon, and carbon filaments (Fig. 12)77. Adding less than
1 wt.% of other salts, such as SnCl2 or PbCl2, results in the formation
of metal nanowires coated with amorphous carbon77,79,80. So far,
only the generation of MWNTs (MWNTELE) has been reported. The
formation of SWNTs via electrolysis has not been observed. MWNTELE
possess diameters of 10-20 nm, consist of only a few walls, e.g. 10-15,
and are estimated to be >500 nm long. MWNTELE occur predominantly
in entangled bundles also containing amorphous carbon, spheroidal
carbon particles, and metal-encapsulated particles.
Several other production methods for CNTs have been reported.
These processes are often based on earlier concepts and the number of
publications constitutes a minor contribution to the literature.
To summarize, the structure and properties of CNTs are highly
sensitive to the production method and synthesis parameters such as
temperature, reactor size, gas flow and pressure, precursors, etc. For
example, MWNTARC are highly crystalline, have few defects, and are
straight, whereas MWNTCVD are longer, exhibit larger diameters, are
highly defective, and are not straight. Defects influence not only the
electronic structure but also the mechanical properties81. This may
help to understand why the Youngs modulus of MWNTCVD is orders of
magnitude smaller than the Youngs modulus of MWNTARC (Table1).
Characterization and purificationMany groups specialize in the analytical characterization of specific
properties, such as field emission, Raman spectroscopy, conductivity
measurements, and mechanical testing. Other labs use CNTs to
develop products, such as composite materials, flat-panel displays, or
atomic force microscopy tips. Often these research groups do not have
expertise in the production of CNT materials themselves, but purchase
CNTs that are readily available from numerous spin-off companies.
In order to test the quality of commercial CNT material, I randomly
chose several companies and tried to compare their CNT materials
using the information provided.Fig. 13shows images of MWNT
samples from the webpages of four different companies. While all four
samples are sold as MWNTs, it is obvious that the morphology of the
CNT material is very different. In addition, the micrographs are taken
using different microscopy techniques, e.g. TEM and scanning electronmicroscopy (SEM), and at different magnifications.
To illustrate that a single electron microscopy image is not enough
for CNT characterization, I show TEM and SEM images of one sample
labeled SWNTCVD at a range of magnifications (Figs.14 and 15).
At higher magnification, the TEM image depicts double- and triple-
walled nanotubes. Thus, the sample, although labeled SWNTCVD,
is in fact a collection of SWNTs, DWNTs, MWNTs, metal catalyst
particles, and soot, as can be seen clearly at lower magnification.
SEM images taken at lower magnification reveal that the SWNTCVD
material occurs as large agglomerates rather than individual nanotubes.
Therefore, providing only a single micrograph at a given magnification
Carbon nanotubes becoming clean REVIEW
Fig. 12 Typical TEM viewgraph of an electrolytically produced MWNT sample.(Adapted and reprinted with permission from78. 1995 Nature PublishingGroup.)
Fig. 13 Four randomly chosen images of different nanotube samples labeledMWNTs from supporting information provided by the supplier.
Fig. 14 TEM images of a CNT sample taken at different magnifications. Thesample was labeled as SWNTs by the supplier. At lower magnification, it can beseen that the material contains byproducts such as amorphous carbon, metalencapsulated particles, and graphitic carbon particles. Higher magnificationshows the absence of SWNTs and the presence of double- and triple-walledcarbon nanotubes.
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
7/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-234
is insufficient to characterize the material. It is not possible to judge
the quality of the commercial material discussed above from the
information provided by the companies. Structural specifications areoften descriptive rather than factual. Samples, for instance, are named
split MWNTs, short MWNTs, long MWNTs, curly MWNTs, or
similar. Furthermore, the information provided for different samples
varies. Sometimes TEM, SEM, and Raman data is available, other
samples are characterized by different techniques, such as atomic force
microscopy, and BET surface area, or field-emission measurements.
As a result of poor sample quality and lack of consistent
characterization information, a number of labs have developed
purification and separation techniques to obtain clean nanotube
material and to select nanotubes of specific characteristics82,83.
However, such purification methods often also remove large parts of
the nanotubes themselves. For example, oxidation of MWNTs grown
by arc discharge reduces the sample by 99%84. Other methods, such
as acid treatment or surfactants may damage or functionalize the
nanotube surface, and hence may also alter their properties85.
Therefore, in order to be able to provide researchers with specific
CNT material, one first has to characterize the samples carefully. A
minimum characterization must include the electron microscopic
analysis of material at different length scales including SEM, TEM, and
analytical methods. The production method, including the catalyst
employed, needs to be stated. From the micrographs, approximate CNT
content, typical length and diameter, as well as distribution of length
and diameter should be specified. For SWNTs, chirality distributions
should be made available using optical spectroscopy methods86.
Oxidation resistance data would provide information on the
crystallinity of CNTs, e.g. the higher their oxidation resistance, the less
defects are present. Therefore, a standardized characterization protocol
is vital in order to compare samples objectively87.
Carbon nanotube growth systematicsApplications that take advantage of individual CNT properties require
precise classification of the CNT material. Production methods have
advanced significantly and the quality of catalytically grown CNTs has
improved steadily so that large quantities of fairly clean CNTs can now
be produced. However, structural control has yet to be achieved. One
needs to be able to reproduce CNT material independent of the person
carrying out the experiment and the specifics of the setup.This can only be achieved by understanding the growth of CNTs
as a function of the precursor and catalyst materials, experimental
parameters such as gas flow, pressure, and temperature, and production
method. High-throughput synthesis using a combinatorial approach to
catalyst selection88-90, in conjunction with structural characterization
of the catalyst particles and in situ electron microscopy studies91-97, are
essential to create a better understanding of CNT growth.
Although in situ investigations combined with density functional
theory calculations have suggested that CNT growth catalyzed by Ni
particles is a surface-diffusion-based process94,96, there is still a lack
of consistent atomic-scale data98,99 on nanotube formation for other
transition metals commonly used for nanotube growth. Furthermore,it is still unclear whether carbon dissolves and diffuses through the
metal catalyst particle and then precipitates as a carbon filament,
or whether carbon diffuses on the surface of the catalyst particle, or
whether bulk and surface diffusion compete. Therefore, synergetic
experimental-theoretical studies are essential for the clarification of
growth mechanisms that currently are still based on models originally
postulated for carbon fibers in the 1970s5,100. The findings of classical
catalysis and metal corrosion studies ought to be revisited as a focus
for current investigations. At the same time, unspecific descriptions
of CNT samples need to be replaced by a standardized nomenclature.
The abbreviation MWNT alone is insufficient to describe sample
quality. Since there is a clear difference in CNT samples produced
via different methods, the description ought to at least include the
production method, e.g. MWNTARC for MWNTs grown by arc discharge,
or MWNTCVD for those generated using CVD.
SummaryThe demand for uniform CNTs entails two major challenges that need
to be overcome. One is the reproducibility of specific CNT material
and the second is the transition from lab- to large-scale production.
For this, it is indispensable to establish clear characterization patterns 87
and a standard description of real CNT material.
Acknowledgments
I would like to thank the Royal Society for financial support.
REFERENCES
1. Hughes, T. V., and Chambers, C. R., US Patent 405480, (1889)
2. Schtzenberger P. S. L., C. R. Acad. Sci. (1890) 111, 774
3. Radushkevich, L. V., and Lukyanovich, V. M., Zurn. Fisc. Chim. (1952) 26, 88
4. Oberlin, A., et al., J. Cryst. Growth (1976) 32, 335
REVIEW Carbon nanotubes becoming clean
Fig. 15 SEM images of a CNT sample taken at different magnifications. Thesample was labelled as SWNTs by the supplier. At lower magnification itbecomes apparent that the nanotube material occurs is large agglomeratesrather than individual nanotubes.
8/6/2019 Nanotubes Review. Tiene El Intro y Los Metodos
8/8
JAN-FEB 2007 | VOLUME 10 | NUMBER 1-2
Carbon nanotubes becoming clean REVIEW
5. Hayashi, T., et al.,Carbon (2006) 44, 1130
6. De Jong, K. P., and Geus, J. W., Catal. Rev. (2000) 42, 481
7. Brand, U. J., et al., Practical Metallography-Praktische Metallographie (1999) 36,406
8. Zeng, Z., and Natesan, K., Chem. Mater. (2005) 17, 3794
9. Bernst, R., et al., Materials And Corrosion-Werkstoffe Und Korrosion (2006) 57, 72410. Toh, C. H., et al., Materials At High Temperatures (2003) 20, 527
11. Iijima, S., Nature (1991) 354, 56
12. Krtschmer, W., et al., Nature (1990) 347, 354
13. Ando, Y., and Zhao, X. L., New Diamond Frontier Carbon Technol. (2006) 16, 123
14. Monthioux, M., and Kuznetsov, V. L., Carbon (2006) 44, 1621
15. Zhu, H. W., et al., Science (2002) 296, 884
16. Wang, H., et al., Appl. Phys. Lett. (2006) 88, 213111
17. Hamada, N., et al., Phys. Rev. Lett. (1992) 68, 1579
18. Tersoff, J., and Ruoff, R. S., Phys. Rev. Lett. (1994) 73, 676
19. Burch, H. J., et al., Appl. Phys. Lett. (2006) 89, 143110
20. Avouris, P., and Chen, J., Materials Today(2006) 9 (10), 46
21. Hoenlein, W., et al., Microelectron. Eng. (2006) 83, 619
22. Kreupl, F., et al., Microelectron. Eng. (2002) 64, 399
23. Khlobystov, A. N., et al., J. Mater. Chem. (2004) 14, 2852
24. Wongwiriyapan, W., et al., Nanotechnology(2006) 17, 4424
25. Kong, J., et al., Science (2000) 287, 622
26. Modi, A., et al., Nature (2003) 424, 171
27. Coleman, J. N., et al., Carbon (2006) 44, 1624
28. Thostenson, E. T., et al., J. Phys. D: Appl. Phys. (2005) 38, 3962
29. Poyato, R., et al., Nanotechnology(2006) 17, 1770
30. Kim, K. T., et al., Mater. Sci. Eng., A (2006) 430, 27
31. Harris, P. J. F., Int. Mater. Rev. (2004) 49, 31
32. Fahlman, B. D., Curr. Org. Chem. (2006) 10, 1021
33. Sato, H., and Hata, K., New Diamond Frontier Carbon Technol. (2006) 16, 163
34. Bell, M. S., et al., Carbon: The Future Material For Advanced TechnologyApplications, Messina, G., et al. (eds.), Springer-Verlag, Berlin (2006) 100, 77
35. Terranova, M. L., et al., Chemical Vapor Deposition (2006) 12, 315
36. Ebbesen, T. W., and Ajayan, P. M., Nature (1992) 358, 220
37. Journet, C., et al., Nature (1997) 388, 756
38. Blase, X., et al., Phys. Rev. Lett. (1999) 83, 5078
39. Li, L.-J., et al., Carbon (2006) 44, 2752
40. Wang, Z. Y., et al., Prog. Chem. (2006) 18, 563
41. Loiseau, A., and Willaime, F., Appl. Surf. Sci. (2000) 164, 227
42. Demoncy, N., et al., Eur. Phys. J. B (1998) 4, 147
43. Loiseau, A., and Pascard, H., Chem. Phys. Lett. (1996) 256, 246
44. Dillon, A. C., et al., Chem. Phys. Lett. (2000) 316, 13
45. Braidy, N., et al., Chem. Phys. Lett. (2002) 354, 88
46. Scott, C. D., et al., Appl. Phys. A (2001) 72, 573
47. Guo, T., et al., Chem. Phys. Lett. (1995) 243, 49
48. Endo, M., CHEMTECH (1988) 18, 568
49. Grobert, N., et al., Chem. Commun. (2001), 47150. Nasibulin, A. G., et al., J. Nanoparticle Res. (2006) 8, 465
51. Ku, B. K., et al., Nanotechnology(2006) 17, 3613
52. Pinault, M., et al., Nano Lett. (2005) 5, 2394
53. Mayne, M., et al., Chem. Phys. Lett. (2001) 338, 101
54. Reyes-Reyes, M., et al., Chem. Phys. Lett. (2004) 396, 167
55. Kamalakaran, R., et al., Carbon (2003) 41, 2737
56. Kondo, D., et al., Chem. Phys. Lett. (2006) 422, 481
57. Zhong, G. F., et al., Jpn. J. Appl. Phys. (2005) 44, 1558
58. Kiselev, N. A., et al., Carbon (2006) 44, 2289
59. Flahaut, E., Chem. Commun. (2003), 1442
60. Park, D., et al., Carbon (2003) 41, 1025
61. Kuang, M. H., et al., Appl. Phys. Lett. (2000) 76, 1255
62. Sunden, E., et al.,J. Vac. Sci. Technol., B (2006) 24, 1947
63. Terrones, M., et al., Nature (1997) 388, 52
64. Grobert, N., et al., Appl. Phys. A (2000) 70, 175
65. Chen, M. Y., et al., J. Electrochem. Soc. (2006) 153, C747
66. Kim, H. S., et al., On The Convergence Of Bio-Information-, Environmental-,Energy-, Space- And Nano-Technologies, Pts 1 & 2 (2005) 277-279, 950
67. Kim, J., et al., J. Appl. Phys. (2001) 90, 2591
68. Grobert, N., DPhil Thesis, University of Sussex, UK, (2000)
69. Amelinckx, S., et al., Science (1994) 265, 635
70. Lau, K. T., et al., Compos. B - Eng. (2006) 37, 437
71. Wang, W. L., et al.,J. Am. Chem. Soc. (2006) 128, 6530
72. Ewels, C. P., and Glerup, M., J. Nanosci. Nanotechnol. (2005) 5, 1345
73. Lozano-Castell, D., et al., Carbon (2004) 42, 2223
74. Terrones, M., et al., Carbon (2002) 40, 1665
75. Trasobares, S., et al., J. Chem. Phys. (2002) 116, 8966
76. Trasobares, S., et al., Eur. Phys. J. B (2001) 22, 117
77. Hsu, W. K., et al., Chem. Phys. Lett. (1996) 262, 161
78. Hsu, W. K., et al., Nature (1995) 377, 687
79. Hsu, W. K., et al., Chem. Mater. (1999) 11, 1747
80. Hsu, W. K., et al., Chem. Phys. Lett. (1999) 301, 159
81. Yu, M.-F. J. Eng. Mater. Technol. (2004) 126, 271
82. Bonard, J.-M., et al., Adv. Mater. (1997) 9, 827
83. Liu, X. M., et al., Curr. Appl. Phys. (2006) 6, 427
84. Ebbesen, T. W., et al., Nature (1994) 367, 519
85. Banerjee, S., and Wong, S. S., J. Phys. Chem. B (2002) 106, 12144
86. Bachilo, S. M., et al., Science (2002) 298, 2361
87. Grobert, N., et al., (2006), in preparation
88. Noda, S., et al., Carbon (2006) 44, 1414
89. Noda, S., et al., Appl. Phys. Lett. (2005) 86, 173106
90. Kakehi, K., et al., Chem. Phys. Lett. (2006) 428, 38191. Sharma, R., and Iqbal, Z., Appl. Phys. Lett. (2004) 84, 990
92. Hansen, P. L., et al., Adv. Catal. (2006) 50, 77
93. Sehested, J., et al., Appl. Catal., A (2006) 309, 237
94. Abild-Pedersen, F., et al., Phys. Rev. B (2006) 73, 115419
95. Helveg, S., and Hansen, P. L., Catalysis Today(2006) 111, 68
96. Helveg, S., et al., Nature (2004) 427, 426
97. Sharma, R., J. Mater. Res. (2005) 20, 1695
98. Raty, J.-Y., et al., Phys. Rev. Lett. (2005) 95, 096103
99. Amara, H., et al., Phys. Rev. B (2006) 73, 113404
100. Dresselhaus, M. S., et al., Graphite Fibers and Filaments. Springer-Verlag, Berlin(1988) 5
101. Terrones, M., et al., Nanotubes: A revolution in materials science and electronics.In Fullerenes And Related Structures, Hirsch, A (ed.), Springer-Verlag, Berlin(1999) 199, 189
102. Treacy, M. M. J., et al., Nature (1996) 381, 678
103. Krishnan, A., et al., Phys. Rev. B (1998) 58, 14013
104. Wong, E. W., et al., Science (1997) 277, 1971
105. Salvetat, J.-P., et al., Appl. Phys. A (1999) 69, 255
106. Salvetat, J.-P., et al., Adv. Mater. (1999) 11, 161
107. Yu, M.-F., et al., Science (2000) 287, 637
108. Demczyk, B. G., et al., Mater. Sci. Eng., A (2002) 334, 173
109. Bacon, R., J. Appl. Phys. (1960) 31, 283
110. Edie, D. D., McHugh, J. J., In Carbon materials for Advanced Technologies, Burchill,T., (ed.), Pergammon, Amsterdam, (1999), 134