Carbon nanotube

A carbon nanotube (CNT) is a tube made of carbon with diameters typically measured in nanometers.

A scanning tunneling microscopy image of a single-walled carbon nanotube
Rotating single-walled zigzag carbon nanotube

Single-wall carbon nanotubes (SWCNTs) are one of the allotropes of carbon, intermediate between fullerene cages and flat graphene, with diameters in the range of a nanometre. Although not made this way, single-wall carbon nanotubes can be idealized as cutouts from a two-dimensional hexagonal lattice of carbon atoms rolled up along one of the Bravais lattice vectors of the hexagonal lattice to form a hollow cylinder. In this construction, periodic boundary conditions are imposed over the length of this roll-up vector to yield a helical lattice of seamlessly bonded carbon atoms on the cylinder surface.[1]

Multi-wall carbon nanotubes (MWCNTs) consisting of nested single-wall carbon nanotubes[1] weakly bound together by van der Waals interactions in a tree ring-like structure. If not identical, these tubes are very similar to Oberlin, Endo, and Koyama's long straight and parallel carbon layers cylindrically arranged around a hollow tube.[2] Multi-wall carbon nanotubes are also sometimes used to refer to double- and triple-wall carbon nanotubes.

Carbon nanotubes can also refer to tubes with an undetermined carbon-wall structure and diameters less than 100 nanometres. Such tubes were discovered in 1952 by Radushkevich and Lukyanovich.[3][4]

The length of a carbon nanotube produced by common production methods is often not reported, but is typically much larger than its diameter. Thus, for many purposes, end effects are neglected and the length of carbon nanotubes is assumed infinite.

Carbon nanotubes can exhibit remarkable electrical conductivity,[5][6] while others are semiconductors.[7][8] They also have exceptional tensile strength[9] and thermal conductivity[10][11][12] because of their nanostructure and strength of the bonds between carbon atoms. In addition, they can be chemically modified.[13] These properties are expected to be valuable in many areas of technology, such as electronics, optics, composite materials (replacing or complementing carbon fibers), nanotechnology, and other applications of materials science.

Rolling up a hexagonal lattice along different directions to form different infinitely long single-wall carbon nanotubes shows that all of these tubes not only have helical but also translational symmetry along the tube axis and many also have nontrivial rotational symmetry about this axis. In addition, most are chiral, meaning the tube and its mirror image cannot be superimposed. This construction also allows single-wall carbon nanotubes to be labeled by a pair of integers.[7]

A special group of achiral single-wall carbon nanotubes are metallic,[5] but all the rest are either small or moderate band gap semiconductors.[7] These electrical properties, however, do not depend on whether the hexagonal lattice is rolled from its back to front or from its front to back and hence are the same for the tube and its mirror image.[7]

The remarkable properties predicted for SWCNTs were tantalizing, but a path to creating them was lacking until 1993, when Iijima and Ichihashi at NEC and Bethune et al. at IBM independently discovered that co-vaporizing carbon and transition metals such as iron and cobalt could specifically catalyze SWCNT formation.[14][15] These discoveries triggered research that succeeded in greatly increasing the efficiency of the catalytic production technique,[16] and led to an explosion of work to characterize and find applications for SWCNTs.

Structure of SWNTs

Zigzag nanotube, configuration (8, 0)
Armchair nanotube, configuration (4, 4)

Basic details

A "sliced and unrolled" representation of a carbon nanotube as a strip of a graphene molecule, overlaid on diagram of the full molecule (faint background). The arrow shows the gap A2 where the atom A1 on one edge of the strip would fit in the opposite edge, as the strip is rolled up
The basis vectors u and v of the relevant sub-lattice, the (n,m) pairs that define non-isomorphic carbon nanotube structures (red dots), and the pairs that define the enantiomers of the chiral ones (blue dots)

The structure of an ideal (infinitely long) single-walled carbon nanotube is that of a regular hexagonal lattice drawn on an infinite cylindrical surface, whose vertices are the positions of the carbon atoms. Since the length of the carbon-carbon bonds is fairly fixed, there are constraints on the diameter of the cylinder and the arrangement of the atoms on it.[17]

In the study of nanotubes, one defines a zigzag path on a graphene-like lattice as a path that turns 60 degrees, alternating left and right, after stepping through each bond. It is also conventional to define an armchair path as one that makes two left turns of 60 degrees followed by two right turns every four steps. On some carbon nanotubes, there is a closed zigzag path that goes around the tube. One says that the tube is of the zigzag type or configuration, or simply is a zigzag nanotube. If the tube is instead encircled by a closed armchair path, it is said to be of the armchair type, or an armchair nanotube. An infinite nanotube that is of the zigzag (or armchair) type consists entirely of closed zigzag (or armchair) paths, connected to each other.

The zigzag and armchair configurations are not the only structures that a single-walled nanotube can have. To describe the structure of a general infinitely long tube, one should imagine it being sliced open by a cut parallel to its axis, that goes through some atom A, and then unrolled flat on the plane, so that its atoms and bonds coincide with those of an imaginary graphene sheet—more precisely, with an infinitely long strip of that sheet. The two halves of the atom A will end up on opposite edges of the strip, over two atoms A1 and A2 of the graphene. The line from A1 to A2 will correspond to the circumference of the cylinder that went through the atom A, and will be perpendicular to the edges of the strip. In the graphene lattice, the atoms can be split into two classes, depending on the directions of their three bonds. Half the atoms have their three bonds directed the same way, and half have their three bonds rotated 180 degrees relative to the first half. The atoms A1 and A2, which correspond to the same atom A on the cylinder, must be in the same class. It follows that the circumference of the tube and the angle of the strip are not arbitrary, because they are constrained to the lengths and directions of the lines that connect pairs of graphene atoms in the same class.

Let u and v be two linearly independent vectors that connect the graphene atom A1 to two of its nearest atoms with the same bond directions. That is, if one numbers consecutive carbons around a graphene cell with C1 to C6, then u can be the vector from C1 to C3, and v be the vector from C1 to C5. Then, for any other atom A2 with same class as A1, the vector from A1 to A2 can be written as a linear combination n u + m v, where n and m are integers. And, conversely, each pair of integers (n,m) defines a possible position for A2.[17] Given n and m, one can reverse this theoretical operation by drawing the vector w on the graphene lattice, cutting a strip of the latter along lines perpendicular to w through its endpoints A1 and A2, and rolling the strip into a cylinder so as to bring those two points together. If this construction is applied to a pair (k,0), the result is a zigzag nanotube, with closed zigzag paths of 2k atoms. If it is applied to a pair (k,k), one obtains an armchair tube, with closed armchair paths of 4k atoms.


Chiral nanotube of the (3,1) type
Chiral nanotube of the (1,3) type, mirror image of the (3,1) type
Nanotube of the (2,2) type, the narrowest "armchair" one
Nanotube of the (3,0) type, the narrowest "zigzag" one

Moreover, the structure of the nanotube is not changed if the strip is rotated by 60 degrees clockwise around A1 before applying the hypothetical reconstruction above. Such a rotation changes the corresponding pair (n,m) to the pair (−2m,n+m). It follows that many possible positions of A2 relative to A1 — that is, many pairs (n,m) — correspond to the same arrangement of atoms on the nanotube. That is the case, for example, of the six pairs (1,2), (−2,3), (−3,1), (−1,−2), (2,−3), and (3,−1). In particular, the pairs (k,0) and (0,k) describe the same nanotube geometry. These redundancies can be avoided by considering only pairs (n,m) such that n > 0 and m ≥ 0; that is, where the direction of the vector w lies between those of u (inclusive) and v (exclusive). It can be verified that every nanotube has exactly one pair (n,m) that satisfies those conditions, which is called the tube's type. Conversely, for every type there is a hypothetical nanotube. In fact, two nanotubes have the same type if and only if one can be conceptually rotated and translated so as to match the other exactly. Instead of the type (n,m), the structure of a carbon nanotube can be specified by giving the length of the vector w (that is, the circumference of the nanotube), and the angle α between the directions of u and w, which may range from 0 (inclusive) to 60 degrees clockwise (exclusive). If the diagram is drawn with u horizontal, the latter is the tilt of the strip away from the vertical.

Chirality and mirror symmetry

A nanotube is chiral if it has type (n,m), with m > 0 and mn; then its enantiomer (mirror image) has type (m,n), which is different from (n,m). This operation corresponds to mirroring the unrolled strip about the line L through A1 that makes an angle of 30 degrees clockwise from the direction of the u vector (that is, with the direction of the vector u+v). The only types of nanotubes that are achiral are the (k,0) "zigzag" tubes and the (k,k) "armchair" tubes. If two enantiomers are to be considered the same structure, then one may consider only types (n,m) with 0 ≤ mn and n > 0. Then the angle α between u and w, which may range from 0 to 30 degrees (inclusive both), is called the "chiral angle" of the nanotube.

Circumference and diameter

From n and m one can also compute the circumference c, which is the length of the vector w, which turns out to be:

in picometres. The diameter of the tube is then , that is

also in picometres. (These formulas are only approximate, especially for small n and m where the bonds are strained; and they do not take into account the thickness of the wall.)

The tilt angle α between u and w and the circumference c are related to the type indices n and m by:

where arg(x,y) is the clockwise angle between the X-axis and the vector (x,y); a function that is available in many programming languages as atan2(y,x). Conversely, given c and α, one can get the type (n,m) by the formulas:

which must evaluate to integers.

Physical limits

Narrowest examples

Tube types that are "degenerate" for being too narrow
Degenerate "zigzag" tube type (1,0)
Degenerate "zigzag" tube type (2,0)
Degenerate "armchair" tube type (1,1)
Possibly degenerate chiral tube type (2,1)

If n and m are too small, the structure described by the pair (n,m) will describe a molecule that cannot be reasonably called a "tube", and may not even be stable. For example, the structure theoretically described by the pair (1,0) (the limiting "zigzag" type) would be just a chain of carbons. That is a real molecule, the carbyne; which has some characteristics of nanotubes (such as orbital hybridization, high tensile strength, etc.) — but has no hollow space, and may not be obtainable as a condensed phase. The pair (2,0) would theoretically yield a chain of fused 4-cycles; and (1,1), the limiting "armchair" structure, would yield a chain of bi-connected 4-rings. These structures may not be realizable.

The thinnest carbon nanotube proper is the armchair structure with type (2,2), which has a diameter of 0.3 nm. This nanotube was grown inside a multi-walled carbon nanotube. Assigning of the carbon nanotube type was done by a combination of high-resolution transmission electron microscopy (HRTEM), Raman spectroscopy, and density functional theory (DFT) calculations.[18]

The thinnest freestanding single-walled carbon nanotube is about 0.43 nm in diameter.[19] Researchers suggested that it can be either (5,1) or (4,2) SWCNT, but the exact type of the carbon nanotube remains questionable.[20] (3,3), (4,3), and (5,1) carbon nanotubes (all about 0.4 nm in diameter) were unambiguously identified using aberration-corrected high-resolution transmission electron microscopy inside double-walled CNTs.[21]



The observation of the longest carbon nanotubes grown so far, around 0.5 metre (550 mm) long, was reported in 2013.[22] These nanotubes were grown on silicon substrates using an improved chemical vapor deposition (CVD) method and represent electrically uniform arrays of single-walled carbon nanotubes.[23]

The shortest carbon nanotube can be considered to be the organic compound cycloparaphenylene, which was synthesized in 2008 by Ramesh Jasti.[24] Other small molecule carbon nanotubes have been synthesized since.[25]


The highest density of CNTs was achieved in 2013, grown on a conductive titanium-coated copper surface that was coated with co-catalysts cobalt and molybdenum at lower than typical temperatures of 450 °C. The tubes averaged a height of 380 nm and a mass density of 1.6 g cm−3. The material showed ohmic conductivity (lowest resistance ~22 kΩ).[26][27]


There is no consensus on some terms describing carbon nanotubes in scientific literature: both "-wall" and "-walled" are being used in combination with "single", "double", "triple", or "multi", and the letter C is often omitted in the abbreviation, for example, multi-walled carbon nanotube (MWNT). The International Standards Organization uses single-wall or multi-wall in its documents.


Triple-walled armchair carbon nanotube

Multi-walled nanotubes (MWNTs) consist of multiple rolled layers (concentric tubes) of graphene. There are two models that can be used to describe the structures of multi-walled nanotubes. In the Russian Doll model, sheets of graphite are arranged in concentric cylinders, e.g., a (0,8) single-walled nanotube (SWNT) within a larger (0,17) single-walled nanotube. In the Parchment model, a single sheet of graphite is rolled in around itself, resembling a scroll of parchment or a rolled newspaper. The interlayer distance in multi-walled nanotubes is close to the distance between graphene layers in graphite, approximately 3.4 Å. The Russian Doll structure is observed more commonly. Its individual shells can be described as SWNTs, which can be metallic or semiconducting. Because of statistical probability and restrictions on the relative diameters of the individual tubes, one of the shells, and thus the whole MWNT, is usually a zero-gap metal.[28]

Double-walled carbon nanotubes (DWNTs) form a special class of nanotubes because their morphology and properties are similar to those of SWNTs but they are more resistant to attacks by chemicals.[29] This is especially important when it is necessary to graft chemical functions to the surface of the nanotubes (functionalization) to add properties to the CNT. Covalent functionalization of SWNTs will break some C=C double bonds, leaving "holes" in the structure on the nanotube and thus modifying both its mechanical and electrical properties. In the case of DWNTs, only the outer wall is modified. DWNT synthesis on the gram-scale by the CCVD technique was first proposed in 2003[30] from the selective reduction of oxide solutions in methane and hydrogen.

The telescopic motion ability of inner shells[31] and their unique mechanical properties[32] will permit the use of multi-walled nanotubes as the main movable arms in upcoming nanomechanical devices. The retraction force that occurs to telescopic motion is caused by the Lennard-Jones interaction between shells, and its value is about 1.5 nN.[33]

Junctions and crosslinking

Transmission electron microscope image of carbon nanotube junction

Junctions between two or more nanotubes have been widely discussed theoretically.[34][35] Such junctions are quite frequently observed in samples prepared by arc discharge as well as by chemical vapor deposition. The electronic properties of such junctions were first considered theoretically by Lambin et al.,[36] who pointed out that a connection between a metallic tube and a semiconducting one would represent a nanoscale heterojunction. Such a junction could therefore form a component of a nanotube-based electronic circuit. The adjacent image shows a junction between two multiwalled nanotubes.

Junctions between nanotubes and graphene have been considered theoretically[37] and studied experimentally.[38] Nanotube-graphene junctions form the basis of pillared graphene, in which parallel graphene sheets are separated by short nanotubes.[39] Pillared graphene represents a class of three-dimensional carbon nanotube architectures.

3D carbon scaffolds

Recently, several studies have highlighted the prospect of using carbon nanotubes as building blocks to fabricate three-dimensional macroscopic (>100 nm in all three dimensions) all-carbon devices. Lalwani et al. have reported a novel radical-initiated thermal crosslinking method to fabricate macroscopic, free-standing, porous, all-carbon scaffolds using single- and multi-walled carbon nanotubes as building blocks.[40] These scaffolds possess macro-, micro-, and nano-structured pores, and the porosity can be tailored for specific applications. These 3D all-carbon scaffolds/architectures may be used for the fabrication of the next generation of energy storage, supercapacitors, field emission transistors, high-performance catalysis, photovoltaics, and biomedical devices, implants, and sensors.[41][42]

Other morphologies

A stable nanobud structure

Carbon nanobuds are a newly created material combining two previously discovered allotropes of carbon: carbon nanotubes and fullerenes. In this new material, fullerene-like "buds" are covalently bonded to the outer sidewalls of the underlying carbon nanotube. This hybrid material has useful properties of both fullerenes and carbon nanotubes. In particular, they have been found to be exceptionally good field emitters.[43] In composite materials, the attached fullerene molecules may function as molecular anchors preventing slipping of the nanotubes, thus improving the composite's mechanical properties.

A carbon peapod[44][45] is a novel hybrid carbon material which traps fullerene inside a carbon nanotube. It can possess interesting magnetic properties with heating and irradiation. It can also be applied as an oscillator during theoretical investigations and predictions.[46][47]

In theory, a nanotorus is a carbon nanotube bent into a torus (doughnut shape). Nanotori are predicted to have many unique properties, such as magnetic moments 1000 times larger than that previously expected for certain specific radii.[48] Properties such as magnetic moment, thermal stability, etc. vary widely depending on the radius of the torus and the radius of the tube.[48][49]

Graphenated carbon nanotubes are a relatively new hybrid that combines graphitic foliates grown along the sidewalls of multiwalled or bamboo style CNTs. The foliate density can vary as a function of deposition conditions (e.g., temperature and time) with their structure ranging from a few layers of graphene (< 10) to thicker, more graphite-like.[50] The fundamental advantage of an integrated graphene-CNT structure is the high surface area three-dimensional framework of the CNTs coupled with the high edge density of graphene. Depositing a high density of graphene foliates along the length of aligned CNTs can significantly increase the total charge capacity per unit of nominal area as compared to other carbon nanostructures.[51]

Cup-stacked carbon nanotubes (CSCNTs) differ from other quasi-1D carbon structures, which normally behave as quasi-metallic conductors of electrons. CSCNTs exhibit semiconducting behavior because of the stacking microstructure of graphene layers.[52]


Many properties of single-walled carbon nanotubes depend significantly on the (n,m) type, and this dependence is non-monotonic (see Kataura plot). In particular, the band gap can vary from zero to about 2 eV and the electrical conductivity can show metallic or semiconducting behavior.


A scanning electron microscopy image of carbon nanotube bundles

Carbon nanotubes are the strongest and stiffest materials yet discovered in terms of tensile strength and elastic modulus. This strength results from the covalent sp2 bonds formed between the individual carbon atoms. In 2000, a multiwalled carbon nanotube was tested to have a tensile strength of 63 gigapascals (9,100,000 psi).[9] (For illustration, this translates into the ability to endure tension of a weight equivalent to 6,422 kilograms-force (62,980 N; 14,160 lbf) on a cable with cross-section of 1 square millimetre (0.0016 sq in)). Further studies, such as one conducted in 2008, revealed that individual CNT shells have strengths of up to ≈100 gigapascals (15,000,000 psi), which is in agreement with quantum/atomistic models.[53] Because carbon nanotubes have a low density for a solid of 1.3 to 1.4 g/cm3,[54] its specific strength of up to 48,000 kN·m·kg−1 is the best of known materials, compared to high-carbon steel's 154 kN·m·kg−1.

Although the strength of individual CNT shells is extremely high, weak shear interactions between adjacent shells and tubes lead to significant reduction in the effective strength of multiwalled carbon nanotubes and carbon nanotube bundles down to only a few GPa.[55] This limitation has been recently addressed by applying high-energy electron irradiation, which crosslinks inner shells and tubes, and effectively increases the strength of these materials to ≈60 GPa for multiwalled carbon nanotubes[53] and ≈17 GPa for double-walled carbon nanotube bundles.[55] CNTs are not nearly as strong under compression. Because of their hollow structure and high aspect ratio, they tend to undergo buckling when placed under compressive, torsional, or bending stress.[56]

On the other hand, there was evidence that in the radial direction they are rather soft. The first transmission electron microscope observation of radial elasticity suggested that even van der Waals forces can deform two adjacent nanotubes. Later, nanoindentations with an atomic force microscope were performed by several groups to quantitatively measure radial elasticity of multiwalled carbon nanotubes and tapping/contact mode atomic force microscopy was also performed on single-walled carbon nanotubes. Young's modulus of on the order of several GPa showed that CNTs are in fact very soft in the radial direction.

It was reported in 2020, CNT-filled polymer nanocomposites with 4 wt% and 6 wt% loadings are the most optimal concentrations, as they provide a good balance between mechanical properties and resilience of mechanical properties against UV exposure for the offshore umbilical sheathing layer.[57]


Band structures computed using tight binding approximation for (6,0) CNT (zigzag, metallic), (10,2) CNT (semiconducting) and (10,10) CNT (armchair, metallic)

Unlike graphene, which is a two-dimensional semimetal, carbon nanotubes are either metallic or semiconducting along the tubular axis. For a given (n,m) nanotube, if n = m, the nanotube is metallic; if nm is a multiple of 3 and n ≠ m, then the nanotube is quasi-metallic with a very small band gap, otherwise the nanotube is a moderate semiconductor.[58] Thus, all armchair (n = m) nanotubes are metallic, and nanotubes (6,4), (9,1), etc. are semiconducting.[59] Carbon nanotubes are not semimetallic because the degenerate point (the point where the π [bonding] band meets the π* [anti-bonding] band, at which the energy goes to zero) is slightly shifted away from the K point in the Brillouin zone because of the curvature of the tube surface, causing hybridization between the σ* and π* anti-bonding bands, modifying the band dispersion.

The rule regarding metallic versus semiconductor behavior has exceptions because curvature effects in small-diameter tubes can strongly influence electrical properties. Thus, a (5,0) SWCNT that should be semiconducting in fact is metallic according to the calculations. Likewise, zigzag and chiral SWCNTs with small diameters that should be metallic have a finite gap (armchair nanotubes remain metallic).[59] In theory, metallic nanotubes can carry an electric current density of 4 × 109 A/cm2, which is more than 1,000 times greater than those of metals such as copper,[60] where for copper interconnects, current densities are limited by electromigration. Carbon nanotubes are thus being explored as interconnects and conductivity-enhancing components in composite materials, and many groups are attempting to commercialize highly conducting electrical wire assembled from individual carbon nanotubes. There are significant challenges to be overcome however, such as undesired current saturation under voltage,[61] and the much more resistive nanotube-to-nanotube junctions and impurities, all of which lower the electrical conductivity of the macroscopic nanotube wires by orders of magnitude, as compared to the conductivity of the individual nanotubes.

Because of its nanoscale cross-section, electrons propagate only along the tube's axis. As a result, carbon nanotubes are frequently referred to as one-dimensional conductors. The maximum electrical conductance of a single-walled carbon nanotube is 2G0, where G0 = 2e2/h is the conductance of a single ballistic quantum channel.[62]

Because of the role of the π-electron system in determining the electronic properties of graphene, doping in carbon nanotubes differs from that of bulk crystalline semiconductors from the same group of the periodic table (e.g., silicon). Graphitic substitution of carbon atoms in the nanotube wall by boron or nitrogen dopants leads to p-type and n-type behavior, respectively, as would be expected in silicon. However, some non-substitutional (intercalated or adsorbed) dopants introduced into a carbon nanotube, such as alkali metals and electron-rich metallocenes, result in n-type conduction because they donate electrons to the π-electron system of the nanotube. By contrast, π-electron acceptors such as FeCl3 or electron-deficient metallocenes function as p-type dopants because they draw π-electrons away from the top of the valence band.

Intrinsic superconductivity has been reported,[63][64][65] although other experiments found no evidence of this, leaving the claim a subject of debate.[66]

In 2021, Michael Strano, the Carbon P. Dubbs Professor of Chemical Engineering at MIT, published department findings on the use of carbon nanotubes to create an electrical current.[67] By immersing the structures in an organic solvent, the liquid drew electrons out of the carbon particles. Strano was quoted as saying, "This allows you to do electrochemistry, but with no wires," and represents a significant breakthrough in the technology.[68] Future applications include powering micro- or nanoscale robots, as well as driving alcohol oxidation reactions, which are important in the chemicals industry.[68]


Carbon nanotubes have useful absorption, photoluminescence (fluorescence), and Raman spectroscopy properties. Spectroscopic methods offer the possibility of quick and non-destructive characterization of relatively large amounts of carbon nanotubes. There is a strong demand for such characterization from the industrial point of view: numerous parameters of nanotube synthesis can be changed, intentionally or unintentionally, to alter the nanotube quality. As shown below, optical absorption, photoluminescence, and Raman spectroscopies allow quick and reliable characterization of this "nanotube quality" in terms of non-tubular carbon content, structure (chirality) of the produced nanotubes, and structural defects. These features determine nearly any other properties such as optical, mechanical, and electrical properties.

Carbon nanotubes are unique "one-dimensional systems" which can be envisioned as rolled single sheets of graphite (or more precisely graphene). This rolling can be done at different angles and curvatures resulting in different nanotube properties. The diameter typically varies in the range 0.4–40 nm (i.e., (X-ray wavelenghts), "only" ~100 times), but the length can vary ~100,000,000,000 times, from 0.14 nm to 55.5 cm.[69] The nanotube aspect ratio, or the length-to-diameter ratio, can be as high as 132,000,000:1,[70] which is unequalled by any other material. Consequently, all the properties of the carbon nanotubes relative to those of typical semiconductors are extremely anisotropic (directionally dependent) and tunable.

Whereas mechanical, electrical, and electrochemical (supercapacitor) properties of the carbon nanotubes are well established and have immediate applications, the practical use of optical properties is yet unclear. The aforementioned tunability of properties is potentially useful in optics and photonics. In particular, light-emitting diodes (LEDs)[71][72] and photo-detectors[73] based on a single nanotube have been produced in the lab. Their unique feature is not the efficiency, which is yet relatively low, but the narrow selectivity in the wavelength of emission and detection of light and the possibility of its fine tuning through the nanotube structure. In addition, bolometer[74] and optoelectronic memory[75] devices have been realised on ensembles of single-walled carbon nanotubes.

Crystallographic defects also affect the tube's electrical properties. A common result is lowered conductivity through the defective region of the tube. A defect in armchair-type tubes (which can conduct electricity) can cause the surrounding region to become semiconducting, and single monatomic vacancies induce magnetic properties.[76]


All nanotubes are expected to be very good thermal conductors along the tube, exhibiting a property known as "ballistic conduction", but good insulators lateral to the tube axis. Measurements show that an individual SWNT has a room-temperature thermal conductivity along its axis of about 3500 W·m−1·K−1;[77] compare this to copper, a metal well known for its good thermal conductivity, which transmits 385 W·m−1·K−1. An individual SWNT has a room-temperature thermal conductivity lateral to its axis (in the radial direction) of about 1.52 W·m−1·K−1,[78] which is about as thermally conductive as soil. Macroscopic assemblies of nanotubes such as films or fibres have reached up to 1500 W·m−1·K−1 so far.[79] Networks composed of nanotubes demonstrate different values of thermal conductivity, from the level of thermal insulation with the thermal conductivity of 0.1 W·m−1·K−1 to such high values.[80] That is dependent on the amount of contribution to the thermal resistance of the system caused by the presence of impurities, misalignments and other factors. The temperature stability of carbon nanotubes is estimated to be up to 2800 °C in vacuum and about 750 °C in air.[81]

Crystallographic defects strongly affect the tube's thermal properties. Such defects lead to phonon scattering, which in turn increases the relaxation rate of the phonons. This reduces the mean free path and reduces the thermal conductivity of nanotube structures. Phonon transport simulations indicate that substitutional defects such as nitrogen or boron will primarily lead to scattering of high-frequency optical phonons. However, larger-scale defects such as Stone–Wales defects cause phonon scattering over a wide range of frequencies, leading to a greater reduction in thermal conductivity.[82]


Techniques have been developed to produce nanotubes in sizeable quantities, including arc discharge, laser ablation, chemical vapor deposition (CVD) and high-pressure carbon monoxide disproportionation (HiPCO). Among these arc discharge, laser ablation, chemical vapor deposition (CVD) are batch by batch process and HiPCO is gas phase continuous process.[83] Most of these processes take place in a vacuum or with process gases. The CVD growth method is popular, as it yields high quantity and has a degree of control over diameter, length and morphology. Using particulate catalysts, large quantities of nanotubes can be synthesized by these methods, but achieving the repeatability becomes a major problem with CVD growth.[84] The HiPCO process advances in catalysis and continuous growth are making CNTs more commercially viable.[85] The HiPCO process helps in producing high purity single walled carbon nanotubes in higher quantity. The HiPCO reactor operates at high temperature 900-1100 °C and high pressure ~30-50 bar.[86] It uses carbon monoxide as the carbon source and iron pentacarbonyl or nickel tetracarbonyl as a catalyst. These catalysts provide a nucleation site for the nanotubes to grow.[83]

Vertically aligned carbon nanotube arrays are also grown by thermal chemical vapor deposition. A substrate (quartz, silicon, stainless steel, etc.) is coated with a catalytic metal (Fe, Co, Ni) layer. Typically that layer is iron and is deposited via sputtering to a thickness of 1–5 nm. A 10–50 nm underlayer of alumina is often also put down on the substrate first. This imparts controllable wetting and good interfacial properties. When the substrate is heated to the growth temperature (~700 °C), the continuous iron film breaks up into small islands with each island then nucleating a carbon nanotube. The sputtered thickness controls the island size and this in turn determines the nanotube diameter. Thinner iron layers drive down the diameter of the islands and drive down the diameter of the nanotubes grown. The amount of time the metal island can sit at the growth temperature is limited as they are mobile and can merge into larger (but fewer) islands. Annealing at the growth temperature reduces the site density (number of CNT/mm2) while increasing the catalyst diameter.

The as-prepared carbon nanotubes always have impurities such as other forms of carbon (amorphous carbon, fullerene, etc.) and non-carbonaceous impurities (metal used for catalyst).[87][88] These impurities need to be removed to make use of the carbon nanotubes in applications.[89]


CNTs are known to have weak dispersibility in many solvents such as water as a consequence of strong intermolecular p–p interactions. This hinders the processability of CNTs in industrial applications. In order to tackle the issue, various techniques have been developed to modify the surface of CNTs in order to improve their stability and solubility in water. This enhances the processing and manipulation of insoluble CNTs rendering them useful for synthesizing innovative CNT nanofluids with impressive properties that are tunable for a wide range of applications. Chemical routes such as covalent functionalization have been studied extensively, which involves the oxidation of CNTs via strong acids (e.g. sulfuric acid, nitric acid, or a mixture of both) in order to set the carboxylic groups onto the surface of the CNTs as the final product or for further modification by esterification or amination. Free radical grafting is a promising technique among covalent functionalization methods, in which alkyl or aryl peroxides, substituted anilines, and diazonium salts are used as the starting agents.

Free radical grafting of macromolecules (as the functional group) onto the surface of CNTs can improve the solubility of CNTs compared to common acid treatments which involve the attachment of small molecules such as hydroxyl onto the surface of CNTs. The solubility of CNTs can be improved significantly by free-radical grafting because the large functional molecules facilitate the dispersion of CNTs in a variety of solvents even at a low degree of functionalization. Recently an innovative environmentally friendly approach has been developed for the covalent functionalization of multi-walled carbon nanotubes (MWCNTs) using clove buds. This approach is innovative and green because it does not use toxic and hazardous acids which are typically used in common carbon nanomaterial functionalization procedures. The MWCNTs are functionalized in one pot using a free radical grafting reaction. The clove-functionalized MWCNTs are then dispersed in water producing a highly stable multi-walled carbon nanotube aqueous suspension (nanofluids).[90]


Computer simulated microstructures with agglomeration regions

Carbon nanotubes are modelled in a similar manner as traditional composites in which a reinforcement phase is surrounded by a matrix phase. Ideal models such as cylindrical, hexagonal and square models are common. The size of the micromechanics model is highly function of the studied mechanical properties. The concept of representative volume element (RVE) is used to determine the appropriate size and configuration of computer model to replicate the actual behavior of CNT reinforced nanocomposite. Depending on the material property of interest (thermal, electrical, modulus, creep), one RVE might predict the property better than the alternatives. While the implementation of ideal model is computationally efficient, they do not represent microstructural features observed in scanning electron microscopy of actual nanocomposites. To incorporate realistic modeling, computer models are also generated to incorporate variability such as waviness, orientation and agglomeration of multiwall or single wall carbon nanotubes.[91]


There are many metrology standards and reference materials available for carbon nanotubes.[92]

For single-wall carbon nanotubes, ISO/TS 10868 describes a measurement method for the diameter, purity, and fraction of metallic nanotubes through optical absorption spectroscopy,[93] while ISO/TS 10797 and ISO/TS 10798 establish methods to characterize the morphology and elemental composition of single-wall carbon nanotubes, using transmission electron microscopy and scanning electron microscopy respectively, coupled with energy dispersive X-ray spectrometry analysis.[94][95]

NIST SRM 2483 is a soot of single-wall carbon nanotubes used as a reference material for elemental analysis, and was characterized using thermogravimetric analysis, prompt gamma activation analysis, induced neutron activation analysis, inductively coupled plasma mass spectroscopy, resonant Raman scattering, UV-visible-near infrared fluorescence spectroscopy and absorption spectroscopy, scanning electron microscopy, and transmission electron microscopy.[96][97] The Canadian National Research Council also offers a certified reference material SWCNT-1 for elemental analysis using neutron activation analysis and inductively coupled plasma mass spectroscopy.[92][98] NIST RM 8281 is a mixture of three lengths of single-wall carbon nanotube.[96][99]

For multiwall carbon nanotubes, ISO/TR 10929 identifies the basic properties and the content of impurities,[100] while ISO/TS 11888 describes morphology using scanning electron microscopy, transmission electron microscopy, viscometry, and light scattering analysis.[101] ISO/TS 10798 is also valid for multiwall carbon nanotubes.[95]

Chemical modification

Carbon nanotubes can be functionalized to attain desired properties that can be used in a wide variety of applications. The two main methods of carbon nanotube functionalization are covalent and non-covalent modifications. Because of their apparent hydrophobic nature,[102] carbon nanotubes tend to agglomerate hindering their dispersion in solvents or viscous polymer melts. The resulting nanotube bundles or aggregates reduce the mechanical performance of the final composite. The surface of the carbon nanotubes can be modified to reduce the hydrophobicity and improve interfacial adhesion to a bulk polymer through chemical attachment.[103]

The surface of carbon nanotubes can be chemically modified by coating spinel nanoparticles by hydrothermal synthesis[104] and can be used for water oxidation purposes.[105]

In addition, the surface of carbon nanotubes can be fluorinated or halofluorinated by heating while in contact with a fluoroorganic substance, thereby forming partially fluorinated carbons (so called Fluocar materials) with grafted (halo)fluoroalkyl functionality.[106][107]


A primary obstacle for applications of carbon nanotubes has been their cost. Prices for single-walled nanotubes declined from around $1500 per gram as of 2000 to retail prices of around $50 per gram of as-produced 40–60% by weight SWNTs as of March 2010. As of 2016, the retail price of as-produced 75% by weight SWNTs was $2 per gram.[108]


Nano tape

Current use and application of nanotubes has mostly been limited to the use of bulk nanotubes, which is a mass of rather unorganized fragments of nanotubes. Bulk nanotube materials may never achieve a tensile strength similar to that of individual tubes, but such composites may, nevertheless, yield strengths sufficient for many applications. Bulk carbon nanotubes have already been used as composite fibers in polymers to improve the mechanical, thermal and electrical properties of the bulk product.

  • Easton-Bell Sports, Inc. have been in partnership with Zyvex Performance Materials, using CNT technology in a number of their bicycle components – including flat and riser handlebars, cranks, forks, seatposts, stems and aero bars.
  • Amroy Europe Oy manufactures Hybtonite carbon nanoepoxy resins where carbon nanotubes have been chemically activated to bond to epoxy, resulting in a composite material that is 20% to 30% stronger than other composite materials. It has been used for wind turbines, marine paints and a variety of sports gear such as skis, ice hockey sticks, baseball bats, hunting arrows, and surfboards.[109]
  • Surrey NanoSystems synthesises carbon nanotubes to create vantablack.
  • "Gecko tape" (also called "nano tape") is often commercially sold as double-sided adhesive tape. It can be used to hang lightweight items such as pictures and decorative items on smooth walls without punching holes in the wall. The carbon nanotube arrays comprising the synthetic setae leave no residue after removal and can stay sticky in extreme temperatures.[110]
  • In tissue engineering, carbon nanotubes have been used as scaffolding for bone growth.[111]
  • Tips for atomic force microscope probes.[112]

Under development

Current research for modern applications include:

  • Utilizing carbon nanotubes as the channel material of carbon nanotube field-effect transistors.[113]
  • Using carbon nanotubes as a scaffold for diverse microfabrication techniques.[114]
  • Energy dissipation in self-organized nanostructures under influence of an electric field.[115]
  • Using carbon nanotubes for environmental monitoring due to their active surface area and their ability to absorb gases.[116]
  • Jack Andraka used carbon nanotubes in his pancreatic cancer test. His method of testing won the Intel International Science and Engineering Fair Gordon E. Moore Award in the spring of 2012.[117]
  • The Boeing Company has patented the use of carbon nanotubes for structural health monitoring[118] of composites used in aircraft structures. This technology will greatly reduce the risk of an in-flight failure caused by structural degradation of aircraft.
  • Zyvex Technologies has also built a 54' maritime vessel, the Piranha Unmanned Surface Vessel, as a technology demonstrator for what is possible using CNT technology. CNTs help improve the structural performance of the vessel, resulting in a lightweight 8,000 lb boat that can carry a payload of 15,000 lb over a range of 2,500 miles.[119]
  • IMEC is using carbon nanotubes for pellicles in semiconductor lithography.[120]

Carbon nanotubes can serve as additives to various structural materials. For instance, nanotubes form a tiny portion of the material(s) in some (primarily carbon fiber) baseball bats, golf clubs, car parts, or damascus steel.[121][122]

IBM expected carbon nanotube transistors to be used on Integrated Circuits by 2020.[123]


The strength and flexibility of carbon nanotubes makes them of potential use in controlling other nanoscale structures, which suggests they will have an important role in nanotechnology engineering.[124] The highest tensile strength of an individual multi-walled carbon nanotube has been tested to be 63 GPa.[9] Carbon nanotubes were found in Damascus steel from the 17th century, possibly helping to account for the legendary strength of the swords made of it.[125][126] Recently, several studies have highlighted the prospect of using carbon nanotubes as building blocks to fabricate three-dimensional macroscopic (>1mm in all three dimensions) all-carbon devices. Lalwani et al. have reported a novel radical initiated thermal crosslinking method to fabricated macroscopic, free-standing, porous, all-carbon scaffolds using single- and multi-walled carbon nanotubes as building blocks.[40] These scaffolds possess macro-, micro-, and nano- structured pores and the porosity can be tailored for specific applications. These 3D all-carbon scaffolds/architectures may be used for the fabrication of the next generation of energy storage, supercapacitors, field emission transistors, high-performance catalysis,[127] photovoltaics, and biomedical devices and implants.

CNTs are potential candidates for future via and wire material in nano-scale VLSI circuits. Eliminating electromigration reliability concerns that plague today's Cu interconnects, isolated (single and multi-wall) CNTs can carry current densities in excess of 1000 MA/cm2 without electromigration damage.[128]

Single-walled nanotubes are likely candidates for miniaturizing electronics. The most basic building block of these systems is an electric wire, and SWNTs with diameters of an order of a nanometre can be excellent conductors.[129][130] One useful application of SWNTs is in the development of the first intermolecular field-effect transistors (FET). The first intermolecular logic gate using SWCNT FETs was made in 2001.[131] A logic gate requires both a p-FET and an n-FET. Because SWNTs are p-FETs when exposed to oxygen and n-FETs otherwise, it is possible to expose half of an SWNT to oxygen and protect the other half from it. The resulting SWNT acts as a not logic gate with both p- and n-type FETs in the same molecule.

Large quantities of pure CNTs can be made into a freestanding sheet or film by surface-engineered tape-casting (SETC) fabrication technique which is a scalable method to fabricate flexible and foldable sheets with superior properties.[132][133] Another reported form factor is CNT fiber (a.k.a. filament) by wet spinning.[134] The fiber is either directly spun from the synthesis pot or spun from pre-made dissolved CNTs. Individual fibers can be turned into a yarn. Apart from its strength and flexibility, the main advantage is making an electrically conducting yarn. The electronic properties of individual CNT fibers (i.e. bundle of individual CNT) are governed by the two-dimensional structure of CNTs. The fibers were measured to have a resistivity only one order of magnitude higher than metallic conductors at 300K. By further optimizing the CNTs and CNT fibers, CNT fibers with improved electrical properties could be developed.[128][135]

CNT-based yarns are suitable for applications in energy and electrochemical water treatment when coated with an ion-exchange membrane.[136] Also, CNT-based yarns could replace copper as a winding material. Pyrhönen et al. (2015) have built a motor using CNT winding.[137][138]

Safety and health

The National Institute for Occupational Safety and Health (NIOSH) is the leading United States federal agency conducting research and providing guidance on the occupational safety and health implications and applications of nanomaterials. Early scientific studies have indicated that nanoscale particles may pose a greater health risk than bulk materials due to a relative increase in surface area per unit mass. Increase in length and diameter of CNT is correlated to increased toxicity[139] and pathological alterations in lung.[140] The biological interactions of nanotubes are not well understood, and the field is open to continued toxicological studies. It is often difficult to separate confounding factors, and since carbon is relatively biologically inert, some of the toxicity attributed to carbon nanotubes may be instead due to residual metal catalyst contamination. In previous studies, only Mitsui-7 was reliably demonstrated to be carcinogenic, although for unclear/unknown reasons.[141] Unlike many common mineral fibers (such as asbestos), most SWCNTs and MWCNTs do not fit the size and aspect-ratio criteria to be classified as respirable fibers. In 2013, given that the long-term health effects have not yet been measured, NIOSH published a Current Intelligence Bulletin[142] detailing the potential hazards and recommended exposure limit for carbon nanotubes and fibers.[143] The U.S. National Institute for Occupational Safety and Health has determined non-regulatory recommended exposure limits (RELs) of 1 μg/m3 for carbon nanotubes and carbon nanofibers as background-corrected elemental carbon as an 8-hour time-weighted average (TWA) respirable mass concentration.[144] It must be noted that although CNT caused pulmonary inflammation and toxicity in mice, exposure to aerosols generated from sanding of composites containing polymer-coated MWCNTs, representative of the actual end-product, did not exert such toxicity.[145]

As of October 2016, single wall carbon nanotubes have been registered through the European Union's Registration, Evaluation, Authorization and Restriction of Chemicals (REACH) regulations, based on evaluation of the potentially hazardous properties of SWCNT. Based on this registration, SWCNT commercialization is allowed in the EU up to 10 metric tons. Currently, the type of SWCNT registered through REACH is limited to the specific type of single wall carbon nanotubes manufactured by OCSiAl, which submitted the application.[146]


The true identity of the discoverers of carbon nanotubes is a subject of some controversy.[147] A 2006 editorial written by Marc Monthioux and Vladimir Kuznetsov in the journal Carbon described the origin of the carbon nanotube.[4] A large percentage of academic and popular literature attributes the discovery of hollow, nanometre-size tubes composed of graphitic carbon to Sumio Iijima of NEC in 1991. His paper initiated a flurry of excitement and could be credited with inspiring the many scientists now studying applications of carbon nanotubes. Though Iijima has been given much of the credit for discovering carbon nanotubes, it turns out that the timeline of carbon nanotubes goes back much further than 1991.[147]

In 1952, L. V. Radushkevich and V. M. Lukyanovich published clear images of 50 nanometre diameter tubes made of carbon in the Journal of Physical Chemistry Of Russia.[3] This discovery was largely unnoticed, as the article was published in Russian, and Western scientists' access to Soviet press was limited during the Cold War. Monthioux and Kuznetsov mentioned in their Carbon editorial:[4]

The fact is, Radushkevich and Lukyanovich [...] should be credited for the discovery that carbon filaments could be hollow and have a nanometre-size diameter, that is to say for the discovery of carbon nanotubes.

In 1976, Morinobu Endo of CNRS observed hollow tubes of rolled up graphite sheets synthesised by a chemical vapour-growth technique.[2] The first specimens observed would later come to be known as single-walled carbon nanotubes (SWNTs).[148] Endo, in his early review of vapor-phase-grown carbon fibers (VPCF), also reminded us that he had observed a hollow tube, linearly extended with parallel carbon layer faces near the fiber core.[149] This appears to be the observation of multi-walled carbon nanotubes at the center of the fiber.[148] The mass-produced MWCNTs today are strongly related to the VPGCF developed by Endo.[148] In fact, they call it the "Endo-process", out of respect for his early work and patents.[148][150] In 1979, John Abrahamson presented evidence of carbon nanotubes at the 14th Biennial Conference of Carbon at Pennsylvania State University. The conference paper described carbon nanotubes as carbon fibers that were produced on carbon anodes during arc discharge. A characterization of these fibers was given, as well as hypotheses for their growth in a nitrogen atmosphere at low pressures.[151]

In 1981, a group of Soviet scientists published the results of chemical and structural characterization of carbon nanoparticles produced by a thermocatalytical disproportionation of carbon monoxide. Using TEM images and XRD patterns, the authors suggested that their "carbon multi-layer tubular crystals" were formed by rolling graphene layers into cylinders. They speculated that via this rolling, many different arrangements of graphene hexagonal nets are possible. They suggested two such possible arrangements: circular arrangement (armchair nanotube); and a spiral, helical arrangement (chiral tube).[152]

In 1987, Howard G. Tennent of Hyperion Catalysis was issued a U.S. patent for the production of "cylindrical discrete carbon fibrils" with a "constant diameter between about 3.5 and about 70 nanometers..., length 102 times the diameter, and an outer region of multiple essentially continuous layers of ordered carbon atoms and a distinct inner core...."[153]

Helping to create the initial excitement associated with carbon nanotubes were Iijima's 1991 discovery of multi-walled carbon nanotubes in the insoluble material of arc-burned graphite rods;[1] and Mintmire, Dunlap, and White's independent prediction that if single-walled carbon nanotubes could be made, they would exhibit remarkable conducting properties.[5] Nanotube research accelerated greatly following the independent discoveries[14][15] by Iijima and Ichihashi at NEC, and Bethune et al. at IBM, of single-walled carbon nanotubes, and methods to specifically produce them by adding transition-metal catalysts to the carbon in an arc discharge. The arc discharge technique was well known to produce the famed Buckminster fullerene on a preparative scale,[154] and these results appeared to extend the run of accidental discoveries relating to fullerenes. Thess et al.[16] refined this catalytic method by vaporizing the carbon/transition-metal combination in a high temperature furnace. This greatly improved the yield and purity of the SWMTs. The discovery of nanotubes remains a contentious issue. Many believe that Iijima's report in 1991 is of particular importance because it brought carbon nanotubes into the awareness of the scientific community as a whole.[147][148]

In 2020, during archaeological excavation of Keezhadi in Tamil Nadu, India, ~2500-year-old pottery was discovered whose coatings appear to contain carbon nanotubes. The robust mechanical properties of the nanotubes are partially why the coatings have lasted for so many years, say the scientists.[155]

See also


This article incorporates public domain text from National Institute of Environmental Health Sciences (NIEHS) as quoted.

  1. Iijima S (7 November 1991). "Helical microtubules of graphitic carbon". Nature. 354 (6348): 56–58. Bibcode:1991Natur.354...56I. doi:10.1038/354056a0. S2CID 4302490.
  2. Oberlin A, Endo M, Koyama T (March 1976). "Filamentous growth of carbon through benzene decomposition". Journal of Crystal Growth. 32 (3): 335–349. Bibcode:1976JCrGr..32..335O. doi:10.1016/0022-0248(76)90115-9.
  3. Radushkevich LV (1952). О Структуре Углерода, Образующегося При Термическом Разложении Окиси Углерода На Железном Контакте [On the Structure of Carbon Formed During the Thermal Decomposition of Carbon Oxide on an Iron Contact] (PDF). Журнал Физической Химии [Journal of Physical Chemistry] (in Russian). 26: 88–95. Archived from the original (PDF) on 5 March 2016. Retrieved 5 April 2012.
  4. Monthioux M, Kuznetsov VL (August 2006). "Who should be given the credit for the discovery of carbon nanotubes?" (PDF). Carbon. 44 (9): 1621–1623. doi:10.1016/j.carbon.2006.03.019. Archived (PDF) from the original on 9 October 2022.
  5. Mintmire JW, Dunlap BI, White CT (February 1992). "Are fullerene tubules metallic?". Physical Review Letters. 68 (5): 631–634. Bibcode:1992PhRvL..68..631M. doi:10.1103/PhysRevLett.68.631. PMID 10045950.
  6. Tans SJ, Devoret MH, Dai H, Thess A, Smalley RE, Geerligs LJ, Dekker C (April 1997). "Individual single-wall carbon nanotubes as quantum wires". Nature. 386 (6624): 474–477. Bibcode:1997Natur.386..474T. doi:10.1038/386474a0. S2CID 4366705.
  7. Hamada N, Sawada SI, Oshiyama A (March 1992). "New one-dimensional conductors: Graphitic microtubules". Physical Review Letters. 68 (10): 1579–1581. Bibcode:1992PhRvL..68.1579H. doi:10.1103/PhysRevLett.68.1579. PMID 10045167.
  8. Wilder JW, Venema LC, Rinzler AG, Smalley RE, Dekker C (1 January 1998). "Electronic structure of atomically resolved carbon nanotubes". Nature. 391 (6662): 59–62. Bibcode:1998Natur.391...59W. doi:10.1038/34139. S2CID 205003208.
  9. Yu MF, Lourie O, Dyer MJ, Moloni K, Kelly TF, Ruoff RS (January 2000). "Strength and breaking mechanism of multiwalled carbon nanotubes under tensile load". Science. 287 (5453): 637–640. Bibcode:2000Sci...287..637Y. doi:10.1126/science.287.5453.637. PMID 10649994.
  10. Sadri R, Ahmadi G, Togun H, Dahari M, Kazi SN, Sadeghinezhad E, Zubir N (28 March 2014). "An experimental study on thermal conductivity and viscosity of nanofluids containing carbon nanotubes". Nanoscale Research Letters. 9 (1): 151. Bibcode:2014NRL.....9..151S. doi:10.1186/1556-276X-9-151. PMC 4006636. PMID 24678607.
  11. Berber S, Kwon YK, Tomanek D (May 2000). "Unusually high thermal conductivity of carbon nanotubes". Physical Review Letters. 84 (20): 4613–4616. arXiv:cond-mat/0002414. Bibcode:2000PhRvL..84.4613B. doi:10.1103/PhysRevLett.84.4613. PMID 10990753. S2CID 9006722.
  12. Kim P, Shi L, Majumdar A, McEuen PL (November 2001). "Thermal transport measurements of individual multiwalled nanotubes". Physical Review Letters. 87 (21): 215502. arXiv:cond-mat/0106578. Bibcode:2001PhRvL..87u5502K. doi:10.1103/PhysRevLett.87.215502. PMID 11736348. S2CID 12533685.
  13. Karousis N, Tagmatarchis N, Tasis D (September 2010). "Current progress on the chemical modification of carbon nanotubes". Chemical Reviews. 110 (9): 5366–5397. doi:10.1021/cr100018g. PMID 20545303.
  14. Iijima S, Ichihashi T (17 June 1993). "Single-shell carbon nanotubes of 1-nm diameter". Nature. 363 (6430): 603–605. Bibcode:1993Natur.363..603I. doi:10.1038/363603a0. S2CID 4314177.
  15. Bethune DS, Kiang CH, De Vries MS, Gorman G, Savoy R, Vazquez J, Beyers R (17 June 1993). "Cobalt-catalyzed growth of carbon nanotubes with single-atomic-layer walls". Nature. 363 (6430): 605–607. Bibcode:1993Natur.363..605B. doi:10.1038/363605a0. S2CID 4321984.
  16. Thess A, Lee R, Nikolaev P, Dai H, Petit P, Robert J, et al. (July 1996). "Crystalline Ropes of Metallic Carbon Nanotubes". Science. 273 (5274): 483–487. Bibcode:1996Sci...273..483T. doi:10.1126/science.273.5274.483. PMID 8662534. S2CID 13284203.
  17. Sinnott SB, Andrews R (July 2001). "Carbon Nanotubes: Synthesis, Properties, and Applications". Critical Reviews in Solid State and Materials Sciences. 26 (3): 145–249. Bibcode:2001CRSSM..26..145S. doi:10.1080/20014091104189. S2CID 95444574.
  18. Zhao X, Liu Y, Inoue S, Suzuki T, Jones RO, Ando Y (March 2004). "Smallest carbon nanotube is 3 a in diameter" (PDF). Physical Review Letters. 92 (12): 125502. Bibcode:2004PhRvL..92l5502Z. doi:10.1103/PhysRevLett.92.125502. PMID 15089683. Archived (PDF) from the original on 9 October 2022.
  19. Torres-Dias AC (2017). "From mesoscale to nanoscale mechanics in single-wall carbon nanotubes". Carbon. 123: 145–150. doi:10.1016/j.carbon.2017.07.036.
  20. Hayashi T, Kim YA, Matoba T, Esaka M, Nishimura K, Tsukada T, Endo M, Dresselhaus MS (2003). "Smallest Freestanding Single-Walled Carbon Nanotube". Nano Letters. 3 (7): 887–889. Bibcode:2003NanoL...3..887H. doi:10.1021/nl034080r.
  21. Guan L, Suenaga K, Iijima S (February 2008). "Smallest carbon nanotube assigned with atomic resolution accuracy". Nano Letters. 8 (2): 459–462. Bibcode:2008NanoL...8..459G. doi:10.1021/nl072396j. PMID 18186659.
  22. Zhang R, Zhang Y, Zhang Q, Xie H, Qian W, Wei F (July 2013). "Growth of half-meter long carbon nanotubes based on Schulz-Flory distribution". ACS Nano. 7 (7): 6156–6161. doi:10.1021/nn401995z. PMID 23806050.
  23. Wang X, Li Q, Xie J, Jin Z, Wang J, Li Y, et al. (September 2009). "Fabrication of ultralong and electrically uniform single-walled carbon nanotubes on clean substrates". Nano Letters. 9 (9): 3137–3141. Bibcode:2009NanoL...9.3137W. CiteSeerX doi:10.1021/nl901260b. PMID 19650638.
  24. Jasti R, Bhattacharjee J, Neaton JB, Bertozzi CR (December 2008). "Synthesis, characterization, and theory of [9]-, [12]-, and [18]cycloparaphenylene: carbon nanohoop structures". Journal of the American Chemical Society. 130 (52): 17646–17647. doi:10.1021/ja807126u. PMC 2709987. PMID 19055403.
  25. Cheung KY, Segawa Y, Itami K (November 2020). "Synthetic Strategies of Carbon Nanobelts and Related Belt-Shaped Polycyclic Aromatic Hydrocarbons". Chemistry. 26 (65): 14791–14801. doi:10.1002/chem.202002316. PMID 32572996. S2CID 219983922.
  26. "Densest array of carbon nanotubes grown to date". KurzweilAI. 27 September 2013.
  27. Sugime H, Esconjauregui S, Yang J, D'Arsié L, Oliver RA, Bhardwaj S, Cepek C, Robertson J (12 August 2013). "Low temperature growth of ultra-high mass density carbon nanotube forests on conductive supports". Applied Physics Letters. 103 (7): 073116. Bibcode:2013ApPhL.103g3116S. doi:10.1063/1.4818619.
  28. Das S (March 2013). "A review on Carbon nano-tubes – A new era of nanotechnology" (PDF). International Journal of Emerging Technology and Advanced Engineering. 3 (3): 774–781. CiteSeerX Archived (PDF) from the original on 9 October 2022.
  29. Piao Y, Chen CF, Green AA, Kwon H, Hersam MC, Lee CS, Schatz GC, Wang Y (7 July 2011). "Optical and Electrical Properties of Inner Tubes in Outer Wall-Selectively Functionalized Double-Wall Carbon Nanotubes". The Journal of Physical Chemistry Letters. 2 (13): 1577–1582. doi:10.1021/jz200687u.
  30. Flahaut E, Bacsa R, Peigney A, Laurent C (June 2003). "Gram-scale CCVD synthesis of double-walled carbon nanotubes" (PDF). Chemical Communications (12): 1442–1443. doi:10.1039/b301514a. PMID 12841282. S2CID 30627446. Archived (PDF) from the original on 9 October 2022.
  31. Cumings J, Zettl A (July 2000). "Low-friction nanoscale linear bearing realized from multiwall carbon nanotubes". Science. 289 (5479): 602–604. Bibcode:2000Sci...289..602C. CiteSeerX doi:10.1126/science.289.5479.602. PMID 10915618.
  32. Treacy MM, Ebbesen TW, Gibson JM (1996). "Exceptionally high Young's modulus observed for individual carbon nanotubes". Nature. 381 (6584): 678–680. Bibcode:1996Natur.381..678T. doi:10.1038/381678a0. S2CID 4332264.
  33. Zavalniuk V, Marchenko S (2011). "Theoretical analysis of telescopic oscillations in multi-walled carbon nanotubes" (PDF). Low Temperature Physics. 37 (4): 337–342. arXiv:0903.2461. Bibcode:2011LTP....37..337Z. doi:10.1063/1.3592692. S2CID 51932307. Archived (PDF) from the original on 9 October 2022.
  34. Chernozatonskii LA (1992). "Carbon nanotube connectors and planar jungle gyms". Physics Letters A. 172 (3): 173–176. Bibcode:1992PhLA..172..173C. doi:10.1016/0375-9601(92)90978-u.
  35. Menon M, Srivastava D (1 December 1997). "Carbon Nanotube 'T Junctions': Nanoscale Metal-Semiconductor-Metal Contact Devices". Physical Review Letters. 79 (22): 4453–4456. Bibcode:1997PhRvL..79.4453M. doi:10.1103/physrevlett.79.4453.
  36. Lambin P (1996). "Atomic structure and electronic properties of bent carbon nanotubes". Synth. Met. 77 (1–3): 249–1254. doi:10.1016/0379-6779(96)80097-x.
  37. Ma KL (2011). "Electronic transport properties of junctions between carbon nanotubes and graphene nanoribbons". European Physical Journal B. 83 (4): 487–492. Bibcode:2011EPJB...83..487M. doi:10.1140/epjb/e2011-20313-9. S2CID 119497542.
  38. Harris PJ, Suarez-Martinez I, Marks NA (December 2016). "The structure of junctions between carbon nanotubes and graphene shells" (PDF). Nanoscale. 8 (45): 18849–18854. doi:10.1039/c6nr06461b. PMID 27808332. S2CID 42241359. Archived (PDF) from the original on 9 October 2022.
  39. Dimitrakakis GK, Tylianakis E, Froudakis GE (October 2008). "Pillared graphene: a new 3-D network nanostructure for enhanced hydrogen storage". Nano Letters. 8 (10): 3166–3170. Bibcode:2008NanoL...8.3166D. doi:10.1021/nl801417w. PMID 18800853.
  40. Lalwani G, Kwaczala AT, Kanakia S, Patel SC, Judex S, Sitharaman B (March 2013). "Fabrication and Characterization of Three-Dimensional Macroscopic All-Carbon Scaffolds". Carbon. 53: 90–100. doi:10.1016/j.carbon.2012.10.035. PMC 3578711. PMID 23436939.
  41. Lalwani G, Gopalan A, D'Agati M, Sankaran JS, Judex S, Qin YX, Sitharaman B (October 2015). "Porous three-dimensional carbon nanotube scaffolds for tissue engineering". Journal of Biomedical Materials Research. Part A. 103 (10): 3212–3225. doi:10.1002/jbm.a.35449. PMC 4552611. PMID 25788440.
  42. Noyce SG, Vanfleet RR, Craighead HG, Davis RC (March 2019). "High surface-area carbon microcantilevers". Nanoscale Advances. 1 (3): 1148–1154. Bibcode:2019NanoA...1.1148N. doi:10.1039/C8NA00101D. PMC 9418787. PMID 36133213.
  43. Nasibulin AG, Pikhitsa PV, Jiang H, Brown DP, Krasheninnikov AV, Anisimov AS, et al. (March 2007). "A novel hybrid carbon material". Nature Nanotechnology. 2 (3): 156–161. Bibcode:2007NatNa...2..156N. doi:10.1038/nnano.2007.37. PMID 18654245.
  44. Smith BW, Monthioux M, Luzzi DE (1998). "Encapsulated C-60 in carbon nanotubes". Nature. 396 (6709): 323–324. Bibcode:1998Natur.396R.323S. doi:10.1038/24521. S2CID 30670931.
  45. Smith BW, Luzzi DE (2000). "Formation mechanism of fullerene peapods and coaxial tubes: a path to large scale synthesis". Chem. Phys. Lett. 321 (1–2): 169–174. Bibcode:2000CPL...321..169S. doi:10.1016/S0009-2614(00)00307-9.
  46. Su H, Goddard WA, Zhao Y (2006). "Dynamic friction force in a carbon peapod oscillator" (PDF). Nanotechnology. 17 (22): 5691–5695. arXiv:cond-mat/0611671. Bibcode:2006Nanot..17.5691S. doi:10.1088/0957-4484/17/22/026. S2CID 18165997. Archived (PDF) from the original on 9 October 2022.
  47. Wang M, Li CM (January 2010). "An oscillator in a carbon peapod controllable by an external electric field: a molecular dynamics study". Nanotechnology. 21 (3): 035704. Bibcode:2010Nanot..21c5704W. doi:10.1088/0957-4484/21/3/035704. PMID 19966399. S2CID 12358310.
  48. Liu L, Guo GY, Jayanthi CS, Wu SY (May 2002). "Colossal paramagnetic moments in metallic carbon nanotori". Physical Review Letters. 88 (21): 217206. Bibcode:2002PhRvL..88u7206L. doi:10.1103/PhysRevLett.88.217206. PMID 12059501.
  49. Huhtala M, Kuronen A, Kaski K (2002). "Carbon nanotube structures: Molecular dynamics simulation at realistic limit" (PDF). Computer Physics Communications. 146 (1): 30–37. Bibcode:2002CoPhC.146...30H. doi:10.1016/S0010-4655(02)00432-0. Archived from the original (PDF) on 27 June 2008.
  50. Parker CB, Raut AS, Brown B, Stoner BR, Glass JT (2012). "Three-dimensional arrays of graphenated carbon nanotubes". J. Mater. Res. 7. 27 (7): 1046–1053. Bibcode:2012JMatR..27.1046P. doi:10.1557/jmr.2012.43.
  51. Stoner BR, Glass JT (2012). "Carbon nanostructures: a morphological classification for charge density optimization". Diamond and Related Materials. 23: 130–134. Bibcode:2012DRM....23..130S. doi:10.1016/j.diamond.2012.01.034.
  52. Liu Q, Ren W, Chen ZG, Yin L, Li F, Cong H, Cheng HM (2009). "Semiconducting properties of cup-stacked carbon nanotubes" (PDF). Carbon. 47 (3): 731–736. doi:10.1016/j.carbon.2008.11.005. Archived from the original (PDF) on 9 January 2015.
  53. Peng B, Locascio M, Zapol P, Li S, Mielke SL, Schatz GC, Espinosa HD (October 2008). "Measurements of near-ultimate strength for multiwalled carbon nanotubes and irradiation-induced crosslinking improvements". Nature Nanotechnology. 3 (10): 626–631. doi:10.1038/nnano.2008.211. PMID 18839003.
  54. Collins PG, Avouris P (December 2000). "Nanotubes for electronics". Scientific American. 283 (6): 62–69. Bibcode:2000SciAm.283f..62C. doi:10.1038/scientificamerican1200-62. PMID 11103460.
  55. Filleter T, Bernal R, Li S, Espinosa HD (July 2011). "Ultrahigh strength and stiffness in cross-linked hierarchical carbon nanotube bundles". Advanced Materials. 23 (25): 2855–2860. doi:10.1002/adma.201100547. PMID 21538593. S2CID 6363504.
  56. Jensen K, Mickelson W, Kis A, Zettl A (26 November 2007). "Buckling and kinking force measurements on individual multiwalled carbon nanotubes". Physical Review B. 76 (19): 195436. Bibcode:2007PhRvB..76s5436J. doi:10.1103/PhysRevB.76.195436.
  57. Okolo C, Rafique R, Iqbal SS, Saharudin MS, Inam F (June 2020). "Carbon Nanotube Reinforced High Density Polyethylene Materials for Offshore Sheathing Applications". Molecules. 25 (13): 2960. doi:10.3390/molecules25132960. PMC 7412307. PMID 32605124.
  58. Laird EA, Kuemmeth F, Steele GA, Grove-Rasmussen K, Nygård J, Flensberg K, Kouwenhoven LP (2015). "Quantum Transport in Carbon Nanotubes". Reviews of Modern Physics. 87 (3): 703–764. arXiv:1403.6113. Bibcode:2015RvMP...87..703L. doi:10.1103/RevModPhys.87.703. S2CID 119208985.
  59. Lu X, Chen Z (October 2005). "Curved pi-conjugation, aromaticity, and the related chemistry of small fullerenes (< C60) and single-walled carbon nanotubes". Chemical Reviews. 105 (10): 3643–3696. doi:10.1021/cr030093d. PMID 16218563.
  60. Hong S, Myung S (April 2007). "Nanotube electronics: a flexible approach to mobility". Nature Nanotechnology. 2 (4): 207–208. Bibcode:2007NatNa...2..207H. doi:10.1038/nnano.2007.89. PMID 18654263.
  61. Vasylenko A, Wynn J, Medeiros PV, Morris AJ, Sloan J, Quigley D (2017). "Encapsulated nanowires: Boosting electronic transport in carbon nanotubes". Physical Review B. 95 (12): 121408. arXiv:1611.04867. Bibcode:2017PhRvB..95l1408V. doi:10.1103/PhysRevB.95.121408. S2CID 59023024.
  62. Charlier JC, Blase X, Roche S (2007). "Electronic and transport properties of nanotubes" (PDF). Reviews of Modern Physics. 79 (2): 677–732. Bibcode:2007RvMP...79..677C. doi:10.1103/RevModPhys.79.677.
  63. Tang ZK, Zhang L, Wang N, Zhang XX, Wen GH, Li GD, et al. (June 2001). "Superconductivity in 4 angstrom single-walled carbon nanotubes". Science. 292 (5526): 2462–2465. Bibcode:2001Sci...292.2462T. doi:10.1126/science.1060470. PMID 11431560. S2CID 44987798.
  64. Takesue I, Haruyama J, Kobayashi N, Chiashi S, Maruyama S, Sugai T, Shinohara H (February 2006). "Superconductivity in entirely end-bonded multiwalled carbon nanotubes". Physical Review Letters. 96 (5): 057001. arXiv:cond-mat/0509466. Bibcode:2006PhRvL..96e7001T. doi:10.1103/PhysRevLett.96.057001. PMID 16486971. S2CID 119049151.
  65. Lortz R, Zhang Q, Shi W, Ye JT, Ye JT, Qiu C, et al. (May 2009). "Superconducting characteristics of 4-A carbon nanotube-zeolite composite". Proceedings of the National Academy of Sciences of the United States of America. 106 (18): 7299–7303. doi:10.1073/pnas.0813162106. PMC 2678622. PMID 19369206.
  66. Bockrath M (1 March 2006). "The weakest link". Nature Physics. 2 (3): 155–156. doi:10.1038/nphys252. S2CID 125902065.
  67. Liu AT, Kunai Y, Cottrill AL, Kaplan A, Zhang G, Kim H, et al. (June 2021). "Solvent-induced electrochemistry at an electrically asymmetric carbon Janus particle". Nature Communications. 12 (1): 3415. Bibcode:2021NatCo..12.3415L. doi:10.1038/s41467-021-23038-7. PMC 8184849. PMID 34099639. S2CID 235370395.
  68. Trafton A (7 June 2021). "MIT Engineers Have Discovered a Completely New Way of Generating Electricity". SciTechDaily. SciTechDaily. Retrieved 8 June 2021.
  69. Zhang R, Zhang Y, Zhang Q, Xie H, Qian W, Wei F (July 2013). "Growth of half-meter long carbon nanotubes based on Schulz-Flory distribution". ACS Nano. 7 (7): 6156–6161. doi:10.1021/nn401995z. PMID 23806050.
  70. Wang X, Li Q, Xie J, Jin Z, Wang J, Li Y, et al. (September 2009). "Fabrication of ultralong and electrically uniform single-walled carbon nanotubes on clean substrates" (PDF). Nano Letters. 9 (9): 3137–3141. Bibcode:2009NanoL...9.3137W. CiteSeerX doi:10.1021/nl901260b. PMID 19650638. Archived from the original (PDF) on 8 August 2017. Retrieved 24 October 2017.
  71. Misewich JA, Martel R, Avouris P, Tsang JC, Heinze S, Tersoff J (May 2003). "Electrically induced optical emission from a carbon nanotube FET". Science. 300 (5620): 783–786. Bibcode:2003Sci...300..783M. doi:10.1126/science.1081294. PMID 12730598. S2CID 36336745.
  72. Chen J, Perebeinos V, Freitag M, Tsang J, Fu Q, Liu J, Avouris P (November 2005). "Bright infrared emission from electrically induced excitons in carbon nanotubes". Science. 310 (5751): 1171–1174. Bibcode:2005Sci...310.1171C. doi:10.1126/science.1119177. PMID 16293757. S2CID 21960183.
  73. Freitag M, Martin Y, Misewich JA, Martel R, Avouris P (2003). "Photoconductivity of Single Carbon Nanotubes". Nano Letters. 3 (8): 1067–1071. Bibcode:2003NanoL...3.1067F. doi:10.1021/nl034313e.
  74. Itkis ME, Borondics F, Yu A, Haddon RC (April 2006). "Bolometric infrared photoresponse of suspended single-walled carbon nanotube films". Science. 312 (5772): 413–416. Bibcode:2006Sci...312..413I. doi:10.1126/science.1125695. PMID 16627739.
  75. Star A, Lu Y, Bradley K, Grüner G (2004). "Nanotube Optoelectronic Memory Devices". Nano Letters. 4 (9): 1587–1591. Bibcode:2004NanoL...4.1587S. doi:10.1021/nl049337f.
  76. Carbon-Based Magnetism: An Overview of the Magnetism of Metal Free Carbon-based Compounds and Materials, Tatiana Makarova and Fernando Palacio (eds.), Elsevier, 2006
  77. Pop E, Mann D, Wang Q, Goodson K, Dai H (January 2006). "Thermal conductance of an individual single-wall carbon nanotube above room temperature". Nano Letters. 6 (1): 96–100. arXiv:cond-mat/0512624. Bibcode:2006NanoL...6...96P. doi:10.1021/nl052145f. PMID 16402794. S2CID 14874373.
  78. Sinha S, Barjami S, Iannacchione G, Schwab A, Muench G (5 June 2005). "Off-axis thermal properties of carbon nanotube films". Journal of Nanoparticle Research. 7 (6): 651–657. Bibcode:2005JNR.....7..651S. doi:10.1007/s11051-005-8382-9. S2CID 138479725.
  79. Koziol KK, Janas D, Brown E, Hao L (1 April 2017). "Thermal properties of continuously spun carbon nanotube fibres". Physica E. 88: 104–108. Bibcode:2017PhyE...88..104K. doi:10.1016/j.physe.2016.12.011.
  80. Kumanek B, Janas D (May 2019). "Thermal conductivity of carbon nanotube networks: a review". Journal of Materials Science. 54 (10): 7397–7427. Bibcode:2019JMatS..54.7397K. doi:10.1007/s10853-019-03368-0.
  81. Thostenson E, Li C, Chou T (2005). "Nanocomposites in context". Composites Science and Technology. 65 (3–4): 491–51. doi:10.1016/j.compscitech.2004.11.003.
  82. Mingo N, Stewart DA, Broido DA, Srivastava D (2008). "Phonon transmission through defects in carbon nanotubes from first principles". Phys. Rev. B. 77 (3): 033418. Bibcode:2008PhRvB..77c3418M. doi:10.1103/PhysRevB.77.033418. hdl:1813/10898.
  83. Nikolaev P (April 2004). "Gas-phase production of single-walled carbon nanotubes from carbon monoxide: a review of the hipco process". Journal of Nanoscience and Nanotechnology. 4 (4): 307–316. doi:10.1166/jnn.2004.066. PMID 15296221.
  84. Schulz MJ, Shanov VN, Yun Y (2009). Nanomedicine Design of Particles, Sensors, Motors, Implants, Robots, and Devices. Artech House. ISBN 9781596932807.
  85. Takeuchi K, Hayashi T, Kim YA, Fujisawa K, Endo M (February 2014). "The state-of-the-art science and applications of carbon nanotubes". Nanosystems: Physics, Chemistry, Mathematics. 5 (1): 15–24.
  86. Bronikowski MJ, Willis PA, Colbert DT, Smith KA, Smalley RE (July 2001). "Gas-phase production of carbon single-walled nanotubes from carbon monoxide via the HiPco process: A parametric study". Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films. 19 (4): 1800–1805. Bibcode:2001JVSTA..19.1800B. doi:10.1116/1.1380721. S2CID 3846517.
  87. Itkis ME, Perea DE, Niyogi S, Rickard SM, Hamon MA, Hu H, Zhao B, Haddon RC (1 March 2003). "Purity Evaluation of As-Prepared Single-Walled Carbon Nanotube Soot by Use of Solution-Phase Near-IR Spectroscopy". Nano Letters. 3 (3): 309–314. Bibcode:2003NanoL...3..309I. doi:10.1021/nl025926e.
  88. Wang L, Pumera M (October 2014). "Residual metallic impurities within carbon nanotubes play a dominant role in supposedly "metal-free" oxygen reduction reactions". Chemical Communications. 50 (84): 12662–12664. doi:10.1039/C4CC03271C. PMID 25204561.
  89. Eatemadi A, Daraee H, Karimkhanloo H, Kouhi M, Zarghami N, Akbarzadeh A, et al. (13 August 2014). "Carbon nanotubes: properties, synthesis, purification, and medical applications". Nanoscale Research Letters. 9 (1): 393. Bibcode:2014NRL.....9..393E. doi:10.1186/1556-276X-9-393. PMC 4141964. PMID 25170330.
  90. Sadri R, Hosseini M, Kazi SN, Bagheri S, Zubir N, Solangi KH, et al. (October 2017). "A bio-based, facile approach for the preparation of covalently functionalized carbon nanotubes aqueous suspensions and their potential as heat transfer fluids". Journal of Colloid and Interface Science. 504: 115–123. Bibcode:2017JCIS..504..115S. doi:10.1016/j.jcis.2017.03.051. PMID 28531649.
  91. Sanei SH, Doles R, Ekaitis T (2019). "Effect of Nanocomposite Microstructure on Stochastic Elastic Properties: An Finite Element Analysis Study". ASCE-ASME Journal of Risk and Uncertainty in Engineering Systems, Part B: Mechanical Engineering. 5 (3): 030903. doi:10.1115/1.4043410. S2CID 140766023.
  92. Stefaniak AB (2017). "Principal Metrics and Instrumentation for Characterization of Engineered Nanomaterials". In Mansfield E, Kaiser DL, Fujita D, Van de Voorde M (eds.). Metrology and Standardization of Nanotechnology. Wiley-VCH Verlag. pp. 151–174. doi:10.1002/9783527800308.ch8. ISBN 9783527800308.
  93. "ISO/TS 10868:2017 – Nanotechnologies – Characterization of single-wall carbon nanotubes using ultraviolet-visible-near infrared (UV-Vis-NIR) absorption spectroscopy". International Organization for Standardization. Archived from the original on 7 September 2017. Retrieved 6 September 2017.
  94. "ISO/TS 10797:2012 – Nanotechnologies – Characterization of single-wall carbon nanotubes using transmission electron microscopy". International Organization for Standardization. Archived from the original on 7 September 2017. Retrieved 6 September 2017.
  95. "ISO/TS 10798:2011 – Nanotechnologies – Characterization of single-wall carbon nanotubes using scanning electron microscopy and energy dispersive X-ray spectrometry analysis". International Organization for Standardization. Archived from the original on 7 September 2017. Retrieved 6 September 2017.
  96. Fagan J (5 March 2009). "Carbon Nanotube Reference Materials". U.S. National Institute of Standards and Technology. Retrieved 6 September 2017.
  97. "SRM 2483 – Single-Wall Carbon Nanotubes (Raw Soot)". U.S. National Institute of Standards and Technology. Archived from the original on 18 February 2013. Retrieved 6 September 2017.
  98. "SWCNT-1: Single-Wall Carbon Nanotube Certified Reference Material – National Research Council Canada". Canadian National Research Council. 7 November 2014. Retrieved 6 September 2017.
  99. "RM 8281 – Single-Wall Carbon Nanotubes (Dispersed, Three Length-Resolved Populations)". U.S. National Institute of Standards and Technology. Archived from the original on 1 April 2015. Retrieved 6 September 2017.
  100. "ISO/TR 10929:2012 – Nanotechnologies – Characterization of multiwall carbon nanotube (MWCNT) samples". International Organization for Standardization. Archived from the original on 7 September 2017. Retrieved 6 September 2017.
  101. "ISO/TS 11888:2017 –Nanotechnologies – Characterization of multiwall carbon nanotubes – Mesoscopic shape factors". International Organization for Standardization. Archived from the original on 7 September 2017. Retrieved 6 September 2017.
  102. Stando G, Łukawski D, Lisiecki F, Janas D (January 2019). "Intrinsic hydrophilic character of carbon nanotube networks". Applied Surface Science. 463: 227–233. Bibcode:2019ApSS..463..227S. doi:10.1016/j.apsusc.2018.08.206. S2CID 105024629.
  103. Karousis N, Tagmatarchis N, Tasis D (September 2010). "Current progress on the chemical modification of carbon nanotubes". Chemical Reviews. 110 (9): 5366–5397. doi:10.1021/cr100018g. PMID 20545303.
  104. Sahoo P, Shrestha RG, Shrestha LK, Hill JP, Takei T, Ariga K (November 2016). "Surface Oxidized Carbon Nanotubes Uniformly Coated with Nickel Ferrite Nanoparticles". Journal of Inorganic and Organometallic Polymers and Materials. 26 (6): 1301–1308. doi:10.1007/s10904-016-0365-z. S2CID 101287773.
  105. Sahoo P, Tan JB, Zhang ZM, Singh SK, Lu TB (7 March 2018). "Engineering the Surface Structure of Binary/Ternary Ferrite Nanoparticles as High-Performance Electrocatalysts for the Oxygen Evolution Reaction". ChemCatChem. 10 (5): 1075–1083. doi:10.1002/cctc.201701790. S2CID 104164617.
  106. US 10000382, Zaderko A, Vasyl UA, "Method for carbon materials surface modification by the fluorocarbons and derivatives", issued June 19, 2018
  107. "WO16072959 Method for Carbon Materials Surface Modification by the Fluorocarbons and Derivatives". Retrieved 17 September 2018.
  108. "Single wall carbon nanotubes". OCSiAl.
  109. Pagni J (5 March 2010). "Amroy aims to become nano-leader". European Plastics News. Archived from the original on 10 July 2011.
  110. "Carbon nanotube tape stays sticky in extreme temperatures". Nanowerk Newsletter. American Chemical Society. 10 July 2019.
  111. Zanello LP, Zhao B, Hu H, Haddon RC (March 2006). "Bone cell proliferation on carbon nanotubes". Nano Letters. 6 (3): 562–567. Bibcode:2006NanoL...6..562Z. doi:10.1021/nl051861e. PMID 16522063.
  112. "Nanotube Tips". nanoScience instruments. Archived from the original on 27 October 2011.
  113. Noyce SG, Doherty JL, Cheng Z, Han H, Bowen S, Franklin AD (March 2019). "Electronic Stability of Carbon Nanotube Transistors Under Long-Term Bias Stress". Nano Letters. 19 (3): 1460–1466. Bibcode:2019NanoL..19.1460N. doi:10.1021/acs.nanolett.8b03986. PMID 30720283. S2CID 73450707.
  114. "Publications on carbon nanotube applications including scaffold microfabrication". 27 May 2014.
  115. Belkin A, Hubler A, Bezryadin A (February 2015). "Self-assembled wiggling nano-structures and the principle of maximum entropy production". Scientific Reports. 5: 8323. Bibcode:2015NatSR...5E8323B. doi:10.1038/srep08323. PMC 4321171. PMID 25662746.
  116. Tan CW, Tan KH, Ong YT, Mohamed AR, Zein SH, Tan SH (September 2012). "Energy and environmental applications of carbon nanotubes". Environmental Chemistry Letters. 10 (3): 265–273. doi:10.1007/s10311-012-0356-4. S2CID 95369378.
  117. Tucker A. "Jack Andraka, the Teen Prodigy of Pancreatic Cancer". Smithsonian Magazine. Retrieved 2 March 2021.
  118. US 9329021, DeLuca MJ, Felker CJ, Heider D, "System and methods for use in monitoring a structure", published May 3, 2016
  119. "Pirahna USV built using nano-enhanced carbon prepreg". 19 February 2009. Archived from the original on 3 March 2012.
  120. LaPedus, Mark (22 March 2021). "EUV Pellicles Finally Ready". Semiconductor Engineering. Retrieved 13 November 2022.
  121. "Legendary Swords' Sharpness, Strength From Nanotubes, Study Says".
  122. Gullapalli S, Wong MS (2011). "Nanotechnology: A Guide to Nano-Objects" (PDF). Chemical Engineering Progress. 107 (5): 28–32. Archived from the original (PDF) on 13 August 2012. Retrieved 24 November 2011.
  123. Simonite T. "IBM Expects Nanotube Transistor Computer Chips Ready Soon After 2020". MIT Technology Review.
  124. Thomas DJ (June 2018). "Ultrafine graphitised MWCNT nanostructured yarn for the manufacture of electrically conductive fabric". The International Journal of Advanced Manufacturing Technology. 96 (9–12): 3805–3808. doi:10.1007/s00170-017-1320-z. S2CID 115751858.
  125. Sanderson K (2006). "Sharpest cut from nanotube sword". Nature News. doi:10.1038/news061113-11. S2CID 136774602.
  126. Reibold M, Paufler P, Levin AA, Kochmann W, Pätzke N, Meyer DC (November 2006). "Materials: carbon nanotubes in an ancient Damascus sabre". Nature. 444 (7117): 286. Bibcode:2006Natur.444..286R. doi:10.1038/444286a. PMID 17108950. S2CID 4431079.
  127. Valenti G, Boni A, Melchionna M, Cargnello M, Nasi L, Bertoni G, et al. (December 2016). "Co-axial heterostructures integrating palladium/titanium dioxide with carbon nanotubes for efficient electrocatalytic hydrogen evolution". Nature Communications. 7: 13549. Bibcode:2016NatCo...713549V. doi:10.1038/ncomms13549. PMC 5159813. PMID 27941752.
  128. Lienig J, Thiele M (2018). "Mitigating Electromigration in Physical Design". Fundamentals of Electromigration-Aware Integrated Circuit Design. Springer. pp. 138–140. doi:10.1007/978-3-319-73558-0. ISBN 978-3-319-73557-3.
  129. Mintmire JW, Dunlap BI, White CT (February 1992). "Are fullerene tubules metallic?". Physical Review Letters. 68 (5): 631–634. Bibcode:1992PhRvL..68..631M. doi:10.1103/PhysRevLett.68.631. PMID 10045950.
  130. Dekker C (May 1999). "Carbon Nanotubes as Molecular Quantum Wires". Physics Today. 52 (5): 22–28. Bibcode:1999PhT....52e..22D. doi:10.1063/1.882658.
  131. Martel R, Derycke V, Lavoie C, Appenzeller J, Chan KK, Tersoff J, Avouris P (December 2001). "Ambipolar electrical transport in semiconducting single-wall carbon nanotubes". Physical Review Letters. 87 (25): 256805. Bibcode:2001PhRvL..87y6805M. doi:10.1103/PhysRevLett.87.256805. PMID 11736597.
  132. Susantyoko RA, Karam Z, Alkhoori S, Mustafa I, Wu CH, Almheiri S (2017). "A surface-engineered tape-casting fabrication technique toward the commercialisation of freestanding carbon nanotube sheets". Journal of Materials Chemistry A. 5 (36): 19255–19266. doi:10.1039/c7ta04999d.
  133. Karam Z, Susantyoko RA, Alhammadi A, Mustafa I, Wu CH, Almheiri S (June 2018). "Development of Surface-Engineered Tape-Casting Method for Fabricating Freestanding Carbon Nanotube Sheets Containing Fe2O3 Nanoparticles for Flexible Batteries". Advanced Engineering Materials. 20 (6): 1701019. doi:10.1002/adem.201701019. S2CID 139283096.
  134. Behabtu N, Young CC, Tsentalovich DE, Kleinerman O, Wang X, Ma AW, et al. (January 2013). "Strong, light, multifunctional fibers of carbon nanotubes with ultrahigh conductivity". Science. 339 (6116): 182–186. Bibcode:2013Sci...339..182B. doi:10.1126/science.1228061. hdl:1911/70792. PMID 23307737. S2CID 10843825.
  135. Piraux L, Araujo FA, Bui TN, Otto MJ, Issi JP (26 August 2015). "Two-dimensional quantum transport in highly conductive carbon nanotube fibers". Physical Review B. 92 (8): 085428. Bibcode:2015PhRvB..92h5428P. doi:10.1103/PhysRevB.92.085428.
  136. Liu F, Wagterveld RM, Gebben B, Otto MJ, Biesheuvel PM, Hamelers HV (November 2014). "Carbon nanotube yarns as strong flexible conductive capacitive electrodes". Colloid and Interface Science Communications. 3: 9–12. doi:10.1016/j.colcom.2015.02.001.
  137. Pyrhönen J, Montonen J, Lindh P, Vauterin J, Otto M (28 February 2015). "Replacing Copper with New Carbon Nanomaterials in Electrical Machine Windings". International Review of Electrical Engineering. 10 (1): 12. CiteSeerX doi:10.15866/iree.v10i1.5253.
  138. Carbon Nanotube Yarn Rotates Electric Motors at LUT. Youtube
  139. Fraser K, Kodali V, Yanamala N, Birch ME, Cena L, Casuccio G, et al. (December 2020). "Physicochemical characterization and genotoxicity of the broad class of carbon nanotubes and nanofibers used or produced in U.S. facilities". Particle and Fibre Toxicology. 17 (1): 62. doi:10.1186/s12989-020-00392-w. PMC 7720492. PMID 33287860.
  140. Fraser K, Hubbs A, Yanamala N, Mercer RR, Stueckle TA, Jensen J, et al. (December 2021). "Histopathology of the broad class of carbon nanotubes and nanofibers used or produced in U.S. facilities in a murine model". Particle and Fibre Toxicology. 18 (1): 47. doi:10.1186/s12989-021-00440-z. PMC 8686255. PMID 34923995.
  141. Barbarino M, Giordano A (March 2021). "Assessment of the Carcinogenicity of Carbon Nanotubes in the Respiratory System". Cancers. 13 (6): 1318. doi:10.3390/cancers13061318. PMC 7998467. PMID 33804168.
  142. "CDC - NIOSH Numbered Publications: Current Intelligence Bulletins (CIB) - Sorted By Date, Descending Order Without Publication Numbers". Retrieved 9 November 2022.
  143. Howard J (April 2013). "Occupational exposure to carbon nanotubes and nanofibers". Current Intelligence Bulletin. DHHS (NIOSH) Publication. 65. doi:10.26616/NIOSHPUB2013145.
  144. "Current intelligence bulletin 65: occupational exposure to carbon nanotubes and nanofibers". 14 July 2020. doi:10.26616/NIOSHPUB2013145. {{cite journal}}: Cite journal requires |journal= (help)
  145. Bishop, Lindsey; Cena, Lorenzo; Orandle, Marlene; Yanamala, Naveena; Dahm, Matthew M.; Birch, M. Eileen; Evans, Douglas E.; Kodali, Vamsi K.; Eye, Tracy; Battelli, Lori; Zeidler-Erdely, Patti C.; Casuccio, Gary; Bunker, Kristin; Lupoi, Jason S.; Lersch, Traci L. (26 September 2017). "In Vivo Toxicity Assessment of Occupational Components of the Carbon Nanotube Life Cycle To Provide Context to Potential Health Effects". ACS Nano. 11 (9): 8849–8863. doi:10.1021/acsnano.7b03038. ISSN 1936-0851.
  146. "REACH Registration Completed for Single-Wall Carbon Nanotubes". PCI Mag. 16 October 2016. Archived from the original on 24 November 2016. Retrieved 24 November 2016.
  147. Pacios Pujadó M (2012). Carbon Nanotubes as Platforms for Biosensors with Electrochemical and Electronic Transduction. Springer Theses. Springer Heidelberg. pp. xx, 208. doi:10.1007/978-3-642-31421-6. hdl:10803/84001. ISBN 978-3-642-31421-6. S2CID 199491391.
  148. Eklund PC (2007). WTEC Panel Report on 'International Assessment of Research and Development of Carbon Nanotube Manufacturing and Applications' Final Report (PDF) (Report). World Technology Evaluation Center (WTEC). Archived from the original (PDF) on 11 March 2017. Retrieved 5 August 2015.
  149. Oberlin A, Endo M, Koyama T (March 1976). "Filamentous growth of carbon through benzene decomposition" (PDF). Journal of Crystal Growth. 32 (3): 335–349. Bibcode:1976JCrGr..32..335O. doi:10.1016/0022-0248(76)90115-9. Archived (PDF) from the original on 9 October 2022.
  150. JP 1982-58,966, Koyama T, Endo MT, "Method for Manufacturing Carbon Fibers by a Vapor Phase Process", issued 1983
  151. Abrahamson J, Wiles PG, Rhoades BL (January 1999). "Structure of carbon fibres found on carbon arc anodes". Carbon. 37 (11): 1873–1874. doi:10.1016/S0008-6223(99)00199-2.
  152. Missing (1982). "Missing". Izvestiya Akademii Nauk SSSR Metally [Proceedings of the Academy of Sciences of the USSR. Metals] (in Russian). 3: 12–17.
  153. US 4663230, Tennent HG, "Carbon fibrils, method for producing same and compositions containing same", issued 1987-05-05
  154. Krätschmer W, Lamb LD, Fostiropoulos KH, Huffman DR (1990). "Solid C60: a new form of carbon". Nature. 347 (6291): 354–358. Bibcode:1990Natur.347..354K. doi:10.1038/347354a0. S2CID 4359360.
  155. Kokarneswaran M, Selvaraj P, Ashokan T, Perumal S, Sellappan P, Murugan KD, et al. (November 2020). "Discovery of carbon nanotubes in sixth century BC potteries from Keeladi, India". Scientific Reports. 10 (1): 19786. Bibcode:2020NatSR..1019786K. doi:10.1038/s41598-020-76720-z. PMC 7666134. PMID 33188244.
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