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Self arrays

Asher S A, Holtz J, Liu L and Wu Z 1994 Self-assembly motif for creating submicron periodic materials. Polymerized crystalline colloidal arrays J. Am. Chem. Soc. 116 4997-8... [Pg.2693]

Fig. 6. Self-consistent band structure (48 valence and 5 conduction bands) for the hexagonal II arrangement of nanotubes, calculated along different high-symmetry directions in the Brillouin zone. The Fermi level is positioned at the degeneracy point appearing between K-H, indicating metallic behavior for this tubule array[17. ... Fig. 6. Self-consistent band structure (48 valence and 5 conduction bands) for the hexagonal II arrangement of nanotubes, calculated along different high-symmetry directions in the Brillouin zone. The Fermi level is positioned at the degeneracy point appearing between K-H, indicating metallic behavior for this tubule array[17. ...
A variation on the exact soiutions is the so-caiied seif-consistent modei that is explained in simpiest engineering terms by Whitney and Riiey [3-12]. Their modei has a singie hollow fiber embedded in a concentric cylinder of matrix material as in Figure 3-26. That is, only one inclusion is considered. The volume fraction of the inclusion in the composite cylinder is the same as that of the entire body of fibers in the composite material. Such an assumption is not entirely valid because the matrix material might tend to coat the fibers imperfectiy and hence ieave voids. Note that there is no association of this model with any particular array of fibers. Also recognize the similarity between this model and the concentric-cylinder model of Hashin and Rosen [3-8]. Other more complex self-consistent models include those by Hill [3-13] and Hermans [3-14] which are discussed by Chamis and Sendeckyj [3-5]. Whitney extended his model to transversely isotropic fibers [3-15] and to twisted fibers [3-16]. [Pg.147]

FIGURE 15.29 These micrographs show that a block < opolymcr on its own > rystallizes in a chaotic pattern a) nanoscale techniques wcr used to produce the self-assi mbled parallel array o the same copolymer in (b) Such n gular arrays could be used to make ultra-high density memory chips to store information in miniature computers... [Pg.768]

The microtubule-associated proteins MAP2 and tau both have two separate functional regions (Lewis et al., 1989). One is the microtubule-binding site, which nucleates microtubule assembly and controls the rate of elongation (by slowing the rate of assembly). The second functional domain shared by MAP2 and tau is a short C-terminal a-helical sequence that can cross-link microtubules into bundles by self-interaction. This domain has some of the properties of a leucine zipper. Likely it is responsible for the organization of microtubules into dense stable parallel arrays in axons and dendrites (Lewis et al., 1989). [Pg.7]

It is now fairly well established that atomic and few-atom cluster arrays can be generated and trapped in weakly interacting matrices 91), and subsequently scrutinized by various forms of spectroscopy. Up to this time, IR-Raman-UV-visible absorption and emission-esr-MCD-EXAFS-Mossbauer methods have been successfully applied to matrix-cluster samples. It is self-evident that an understanding of the methods of generating and identifying these species is a prerequisite for... [Pg.81]

Fig. 34—Bit pattern media (BPM) or self-ordered magnetic arrays. Fig. 34—Bit pattern media (BPM) or self-ordered magnetic arrays.
Jeoung E., Galow T.H., Schotter J., Bal M., Ursache A., Tuominen M.T., Stafford C.M., Russell T.P., and Rotello V.M. Fabrication and characterization of naoelectrode arrays formes via block copolymers self-assembly, Langmuir, 17, 6396, 2001. [Pg.164]

Sharma N, Top A, Kiick KL et al (2009) One-dimensional gold nanoparticle arrays by electrostatically directed organization using polypeptide self-assembly. Angew Chem Int Ed 48 7078-7082... [Pg.162]


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