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Crystals honeycomb lattice

Single crystals of /S-A1203 are essentially two dimensional conductors. The conducting plane has hexagonal symmetry (honeycomb lattice). This characteristic feature made -alumina a useful model substance for testing atomistic transport theory, for example with the aid of computer simulations. Low dimensionality and high symmetry reduce the computing time of the simulations considerably (e.g., for the calculation of correlation factors of solid solutions). [Pg.379]

Another, less direct, approach to manipulate molecules on a surface is through the use of chemical self-assembly principles derived from X-ray crystallographic work. A two-dimensional hydrogen bonding motif derived from crystal-engineering studies has been used to assemble a two-dimensional honeycomb lattice based on the hydrogen bonded triad motif formed between perylene tetracarboxylic acid diimide (5.1) and melamine (5.2). The honeycomb... [Pg.235]

Graphene is a one-atom-thick planar layer of graphite, where the atoms are packed in a hexagonal ( honeycomb ) crystal lattice. The carbon atoms are sp -bonded with a bond length of 1.42 A. The crystal lattice has two atoms per unit cell, A and B, and it is rotationally symmetric for rotations of 120° around any lattice point. One can view the honeycomb lattice as a triangular Bravais lattice with a basis of two atoms per unit cell. Fig. 2a. [Pg.30]

Figure 19.11 Binding and dissociation dynamics of annexin V trimers on the 2D crystai with p6 symmetry. For exampie, the hoie in the honeycomb lattice indicated by an arrow in the 0 sec image is filled by a trimer diffusing on the crystal surface at 0.5 sec and then dissociates in the next 0.5 sec. Successive images were obtained at 2 fps for a scan area of 150 x 150 nm. ... Figure 19.11 Binding and dissociation dynamics of annexin V trimers on the 2D crystai with p6 symmetry. For exampie, the hoie in the honeycomb lattice indicated by an arrow in the 0 sec image is filled by a trimer diffusing on the crystal surface at 0.5 sec and then dissociates in the next 0.5 sec. Successive images were obtained at 2 fps for a scan area of 150 x 150 nm. ...
On a diamond or honeycomb lattice, described by (1.4.25), or for quartz, a-alumina, etc., in which the crystal structure and the orbital character induce non-negligible angular effects, Fmin is non-zero. [Pg.33]

Work on the production and oxidation of SWNT samples at SRI and other laboratories has led to the observation of very long bundles of these tubes, as can be seen in Fig. 2. In the cleanup and removal of the amorphous carbon in the original sample, the SWNTs self-assemble into aligned cable structures due to van der Waals forces. These structures are akin to the SW nanotube crystals discussed by Tersoff and Ruoff they show that van der Waals forces can flatten tubes of diameter larger than 2.5 nm into a hexagonal cross-sectional lattice or honeycomb structure[17]. [Pg.145]

Fig. 11. Crystal structure of graphite. The unit cell is shaded in green, (a) Top view of the surface layer. The hexagonal surface lattice is defined by two unit vectors u and v in the xy-plane with a length of 246 pm and an angle of 120° forming a honeycomb web of hexagonal rings. The basis of the lattice consists of two carbon atoms a, (white) and /3 (red) with a distance of 142 pm. (b) Perspective view, showing the layered structure. The distance between layers is 2.36 times the next-neighbor distance of atoms within one layer, and the bond between layers is weak. The a-atoms (white) are directly above an a-atom in the layer directly underneath at a distance of 334.8 pm the /3-atoms (red) are over hollow sites (h). The unit vector w is parallel to the z-axis with a length of 669.6pm. Fig. 11. Crystal structure of graphite. The unit cell is shaded in green, (a) Top view of the surface layer. The hexagonal surface lattice is defined by two unit vectors u and v in the xy-plane with a length of 246 pm and an angle of 120° forming a honeycomb web of hexagonal rings. The basis of the lattice consists of two carbon atoms a, (white) and /3 (red) with a distance of 142 pm. (b) Perspective view, showing the layered structure. The distance between layers is 2.36 times the next-neighbor distance of atoms within one layer, and the bond between layers is weak. The a-atoms (white) are directly above an a-atom in the layer directly underneath at a distance of 334.8 pm the /3-atoms (red) are over hollow sites (h). The unit vector w is parallel to the z-axis with a length of 669.6pm.
Figure 2. View of molecular packing arrangement in benzenechromium tricarbonyl-(thiourea)3 complex. The view is down the crystal c-axis, looking down the honeycomb formed by the thiourea lattice. Figure 2. View of molecular packing arrangement in benzenechromium tricarbonyl-(thiourea)3 complex. The view is down the crystal c-axis, looking down the honeycomb formed by the thiourea lattice.
Figure 8. A view of 1,3-CHDMn(CO)3--(thiourea)3 illustrating the polar alignment. The view is down the honeycomb axis of the C 7Stal, and it shows the sideways arrangement of the organometallic in the crystal lattice, unlike the arrangements shown in Figure 2 for the chromium complex. Figure 8. A view of 1,3-CHDMn(CO)3--(thiourea)3 illustrating the polar alignment. The view is down the honeycomb axis of the C 7Stal, and it shows the sideways arrangement of the organometallic in the crystal lattice, unlike the arrangements shown in Figure 2 for the chromium complex.
Graphene is considered bidimensional carbon nanofiller with a one-atom-thick planar sheet of sp -bonded carbon atoms that are densely packed in a honeycomb crystal lattice. It is regarded as one of the thinnest materials with tremendous application potential. Graphene and poly-mer/graphene nanocomposites have remarkable properties, among these ... [Pg.599]

Two-dimensional nanostructures have two dimensions outside of the nanometric size range, such as nanoplates, nanosheets, and nanodisks. Graphene is a typical two-dimensional film, which is composed of a one-atom-thick planar sheet of sp -bonded carbon atoms that are densely packed into a honeycomb crystal lattice. This material exhibits a high electrical conductivity, a high surface area of over 2600 m g , an elevated chemical tolerance, and a broad electrochemical window. Therefore, they were used to form two-dimensional nanocomposites with polymers. The graphene not only increases the electrical conductivity of the polymer, but also enhance its mechanical stability. Conducting polymers with various hierarchical structures have been deposited on... [Pg.125]


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