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Showing papers on "Graphene published in 1995"


Journal ArticleDOI
15 Sep 1995-Science
TL;DR: Field emission of electrons from individually mounted carbon nanotubes has been found to be dramatically enhanced when the nanotube tips are opened by laser evaporation or oxidative etching, in a process that resembles unraveling the sleeve of a sweater.
Abstract: Field emission of electrons from individually mounted carbon nanotubes has been found to be dramatically enhanced when the nanotube tips are opened by laser evaporation or oxidative etching. Emission currents of 0.1 to 1 microampere were readily obtained at room temperature with bias voltages of less than 80 volts. The emitting structures are concluded to be linear chains of carbon atoms, Cn, (n = 10 to 100), pulled out from the open edges of the graphene wall layers of the nanotube by the force of the electric field, in a process that resembles unraveling the sleeve of a sweater.

1,538 citations


Journal ArticleDOI
01 Jan 1995-Carbon
TL;DR: In this article, the vibrational modes of carbon nanotubes are reviewed and the number of these modes is found to depend on the tubule symmetry and not on the diameter.

600 citations


Journal ArticleDOI
03 Mar 1995-Science
TL;DR: A model that postulates a mixture of scroll-shaped and concentric, cylindrical graphene sheets is proposed to explain the microstructure of graphite multishell nanotubes grown by arc discharge and explains clustering in a natural way.
Abstract: A model that postulates a mixture of scroll-shaped and concentric, cylindrical graphene sheets is proposed to explain the microstructure of graphite multishell nanotubes grown by arc discharge. The model is consistent with the observed occurrence of a relatively small number of different chiral angles within the same tubule. The model explains clustering in a natural way and is consistent with the observation of asymmetric (0002) lattice fringe patterns and with the occurrence of singular fringe spacings larger than c/2 (c is the c parameter of graphite) in such patterns. Anisotropic thermal contraction accounts for the 2 to 3 percent increase in the c parameter of nanotubes, compared with bulk graphite, but is too small to explain the singular fringe spacings. The model also explains the formation of multishell closure domes. Nucleation is attributed to the initial formation of a fullerene "dome."

199 citations


Journal ArticleDOI
Thomas W. Ebbesen, Hidefumi Hiura1

143 citations


Journal ArticleDOI
01 Jan 1995-Carbon
TL;DR: In this paper, the structure of single-layer carbon nanotubes has been studied using high-resolution transmission electron microscopy, showing that the properties of these tubes will depend sensitively on their detailed structure.

137 citations



Journal ArticleDOI
TL;DR: Using chemical vapor deposition, nanodispersed silicon has been prepared in carbon at temperatures between 850 and 1050°C as discussed by the authors, showing that the silicon is bonded mostly to carbon neighbors and that large clusters of silicon are not found.
Abstract: Using chemical‐vapor deposition nanodispersed silicon has been prepared in carbon at temperatures between 850 and 1050 °C. Samples with up to 11% atomic silicon in carbon show the same pregraphitic x‐ray‐diffraction pattern as those without silicon. X‐ray‐absorption spectroscopy shows that the silicon is bonded mostly to carbon neighbors and that large clusters of silicon are not found. It is believed that silicon atoms, or small clusters of a few silicon atoms, are located in regions of ‘‘unorganized carbon’’ which separate small regions of organized graphene layers. These materials may have application as electrode materials in advanced rechargeable lithium batteries.

86 citations


Journal ArticleDOI
TL;DR: In this article, the structure of carbon fibres was studied by means of various electron diffraction techniques and by electron microscopy, and it was shown that the tubules are hollow and consist of concentric cylindrical graphene sheets.
Abstract: Carbon fibres prepared by the catalytic decomposition of acetylene over finely dispersed cobalt, supported on amorphous silica, are often helix shaped. The structure of such carbon fibres was studied by means of various electron diffraction techniques and by electron microscopy. It was shown that the tubules are hollow and consist of concentric cylindrical graphene sheets. The diffraction patterns are analysed in detail and compared with theoretically predicted patterns. Good semi-quantitative agreement is found. It is shown that the helices are polygonized; their atomic structure is consistent with models predicted on the basis of molecular dynamics simulations.

76 citations


Journal ArticleDOI
TL;DR: The graphene layers at carbon nanotube cap regions are efficiently cleaved by several oxidants (e.g., KMnO4, OsO4 and RuO4) in acidic solution at 100 °C, but not by stronger oxidants, such as K2Cr2O7-H+ and H2O2H+ as mentioned in this paper.
Abstract: The graphene layers at carbon nanotube cap regions are efficiently cleaved by several oxidants (e.g., KMnO4, OsO4 and RuO4) in acidic solution at 100 °C, but not by stronger oxidants, such as K2Cr2O7–H+ and H2O2–H+.

75 citations


Journal ArticleDOI
01 Jan 1995-Carbon
TL;DR: In this paper, double-walled carbon nanotubes, in which the inner and outer tubes are linked by such hemi-toroidal seals, may be one viable way of overcoming the reactivity at the graphene edges of open-ended tubes to engineer stable and useful graphene nanostructures.

36 citations


Journal ArticleDOI
TL;DR: In this paper, the lattice structure of heat-treated vapor-grown carbon fibers (VGCF) was analyzed using transmission electron microscopy and atomic force microscopy (AFM).
Abstract: New structural features observed in heat-treated vapor-grown carbon fibers (VGCF’s), produced by the thermal decomposition of hydrocarbon vapor, are reported using image analysis of the lattice plane structure observed by transmission electron microscopy (TEM) and atomic force microscopy (AFM). The TEM lattice image of well-ordered graphite fibers (heat-treated VGCF’s at 2800 °C) was treated by a two-dimensional fast Fourier transform, showing sharp bright spots associated with the 002 and 100 lattice planes. The heat-treated VGCF’s consist of a polygonally shaped shell, and the long and short fringe structures in the TEM lattice image reflect the 002 and 100 lattice planes, respectively. From this analysis, new facts about the lattice structure are obtained visually and quantitatively. The 002 lattice planes remain and are highly parallel to each other along the fiber axis, maintaining a uniform interlayer spacing of 3.36 A. The 100 lattice planes are observed to make several inclined angles with the 002 lattice planes relative to the plane normals, caused by the gliding of adjacent graphene layers. This work visually demonstrates coexistence of the graphitic stacking, as well as the gliding of the adjacent graphene layers, with a gliding angle of about 3–20°. These glide planes are one of the dominant stacking defects in heat-treated VGCF’s. On the other hand, turbostratic structural evidence was suggested by AFM observations. The structural model of coexisting graphitic, glide, and turbostratic structures is proposed as a transitional stage to perfect three-dimensional stacking in the graphitization process. These structural features could also occur in common carbons and in carbon nanotubes.

Journal ArticleDOI
TL;DR: In this article, the structures of carbon nanotubes are investigated by cross-sectional high-resolution transmission electron microscopy, and it is shown that polygonal rather than circular or spherical geometries predominate.
Abstract: The structures of carbon nanotubes are investigated by cross-sectional high-resolution transmission electron microscopy. Some results for longitudinal sections are also included. No examples of perfect seamless tubes or of “scroll-type” Archimedean spirals are found; in each case examined, papier m[acaron]he-like aggregates of graphene sheets occur, each of finite extent. There is a strong tendency for the structures to relax, locally at least, towards the three-dimensional structure of graphite. Thus polygonal rather than circular or spherical geometries predominate. Some comments are offered concerning a realistic model for the structures, as well as for understanding the electronic properties of multilayer carbon nanotubules. It is proposed that our specimens grew in an atmosphere rich in single graphene sheets, rather than C60 cages.

Book ChapterDOI
01 Jan 1995
TL;DR: In graphite, the growth of graphite takes place predominantly along the edges of the layers and only very slowly normal to the layers (parallel to the c axis) as discussed by the authors.
Abstract: The paradigm for the structure of graphite is that of a staggered stacking of flat layers of carbon atoms (Figure 6-1). Individual layers, sometimes referred to as graphene sheets,1 are weakly bonded to each other and are composed of strongly bonded carbon atoms at the vertices of a network of regular hexagons in a honeycomb pattern.2 Both the properties and the morphology of graphite reflect its highly anisotropic structure. Due to the strong bonding within layers and the weak bonding between layers, the growth of graphite takes place predominantly along the edges of the layers (perpendicular to the c axis) and only very slowly normal to the layers (parallel to the c axis). As a result of the growth rate anisotropy, the anisotropic surface energy, and the crystallographic symmetry, the expected morphology for graphite crystals is that of tabular hexagonal prisms.3 However, well-formed natural crystals, such as shown in Figure 6-2, are rare,4 and it has been said that near-ideal crystals of graphite may be rarer than diamonds.5 Well-formed, laboratory-grown crystals of graphite are also uncommon. During the 1960s, graphite crystals from Ticonderoga, New York, and Sterling Hill, New Jersey, became a standard of perfection for experiments and for comparison with laboratory-grown crystals.6,7

Journal ArticleDOI
01 Jan 1995-Carbon
TL;DR: In this article, the electrical resistivity along the graphene layers was followed with a contactless method, and the results showed that at 20 °C, the intercalation process is associated with a large decrease of resistivity; the lowest values are observed for stages 8 to 5 formation, and remain nearly constant until stage 1.

Journal ArticleDOI
01 Jan 1995-Carbon
TL;DR: In this paper, a high resolution transmission electron microscopy study of fluorine-intercalated carbon fibers has been carried out on two types of host materials: high-temperature treated pitch-based and PAN-based fibers.

Journal ArticleDOI
TL;DR: In this paper, the authors used scanning tunneling microscopy (STM) to obtain images and currentvoltage (I-V) curves of carbon nanotubes produced by arc discharge of carbon electrodes.
Abstract: Scanning tunneling microscopy (STM) has been used to obtain images and current–voltage (I–V) curves of carbon nanotubes produced by arc discharge of carbon electrodes. The STM I–V curves indicate that carbon nanotubes with diameters from 2.0 to 5.1 nm have a metallic density of states. Using STM, we also observe nanometer‐size graphene sheets which are four graphite layers thick. The STM images of carbon nanotubes are in good agreement with transmission electron microscope images.


Journal ArticleDOI
TL;DR: In this article, the c-axis structures of stage 1 and 2 fluorine-graphite intercalation compounds prepared from highly oriented pyrolytic graphite and natural graphite flake have been analyzed by intensity calculation of (00 l ) diffraction lines for the disordered staging structures.

Journal ArticleDOI
TL;DR: In this paper, an energy-filtering transmission electron microscopy was applied to carbon nanotubes in order to investigate quantitative property of elemental maps obtained by inelastically scattered electrons corresponding to the carbon K-edge.
Abstract: Energy-filtering transmission electron microscopy was applied to carbon nanotubes in order to investigate quantitative property of elemental maps obtained by inelastically scattered electrons corresponding to the carbon K-edge. An 1 MeV high-resolution electron microscope (JEOL, ARM-1000) equipped with a GATAN imaging filter was employed. Because of a cylindrical structure of nanotubes the number of carbon atoms contributing to the image changes across the tube axis. We could detect the contrast difference due to 20 carbon atoms in the carbon distribution image of 6 layers tube. Furthermore, we examined the carbon mapping from a conical tip region with progressive closure of carbon layers, where an intensity profile clearly distinguishes the difference of 6 graphene sheets. From the consideration of signal-to-noise ratio, the detection limit is concluded to be less than 22 carbon atoms in the present experimental conditions.

Journal ArticleDOI
13 Aug 1995