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Nanoscale void

CNT films are also of interest from morphological aspect because their structure provides nanoscale voids within the networks of CNTs. For example, composites with conducting polymers are very interesting both from scientific and technological interests, since we would expect CNTs to give a well-dispersed film. [Pg.178]

This chapter deals with the selective preparation, TEM/EXAFS/XPS characterization and catalysis of mono- and bimetallic nanowires and nanoparticles highly ordered in silica FSM-16, organosilica HMM-1 and mesoporous silica thin films. The mechanism of nanowire formation is discussed with the specific surface-mediated reactions of metal precursors in the restraint of nanoscale void space of mesoporous silica templates. The unique catalytic performances of nanowires and particles occluded in mesoporous cavities are also reviewed in terms of their shape and size dependency in catalysis as well as their unique electronic and magnetic properties for the device application. [Pg.600]

M., and Bartlett, P.N. (2007) Understanding plasmons in nanoscale voids. Nono Letters, 7, 2094-2100. [Pg.321]

Coyle S, Netti MC, Baumberg JJ, Ghanem MA, Birkin PR, Bartlett PN, Whittaker DM (2001) Confined plasmons in metallic nanocavities. Phys Rev Lett 87 176801 Cole RM, Baumberg JJ, Garcia de Abajo FJ, Mahajan S, Abdelsalam M, Bartlett PN (2007) Understanding plasmons in nanoscale voids. Nano Lett 7 2094... [Pg.177]

Pethrick, R. A., Positron aimihilation a probe for nanoscale voids and free volume Prog. Polym. Sci., 22, 1-47 (1997). [Pg.469]

Figure 8.62 Crystal structure of 28 viewed along the a axis showing the pillared layer motif depicted in Figure 8.61(b). The nanoscale voids in the pillared region with dimensions of 8 Ay. 22 A are capable of accommodating three columns of independent [(n-C4Hg)4N] cations which are represented by large open, shaded and cross-hatched circles... Figure 8.62 Crystal structure of 28 viewed along the a axis showing the pillared layer motif depicted in Figure 8.61(b). The nanoscale voids in the pillared region with dimensions of 8 Ay. 22 A are capable of accommodating three columns of independent [(n-C4Hg)4N] cations which are represented by large open, shaded and cross-hatched circles...
Asymmetric membranes often have nanoscale void structure ... [Pg.155]

Figure 3. Schematic representation of the micro- and nanoscale morphology of gel-type (a) and macroreticular (b) resins [13], Level 1 is the representation of the dry materials. Level 2 is the representation of the microporous swollen materials at the same linear scale swelling involves the whole polymeric mass in the gel-type resin (2a) and the macropore walls in the macroreticular resin (2b). The morphology of the swollen polymer mass is similar in both gel-type and macroreticular resins (3a,b). Nanopores are actually formed by the void space surrounding the polymeric chains, as shown in level 4, and are a few nanometer wide. (Reprinted from Ref [12], 2003, with permission from Elsevier.)... Figure 3. Schematic representation of the micro- and nanoscale morphology of gel-type (a) and macroreticular (b) resins [13], Level 1 is the representation of the dry materials. Level 2 is the representation of the microporous swollen materials at the same linear scale swelling involves the whole polymeric mass in the gel-type resin (2a) and the macropore walls in the macroreticular resin (2b). The morphology of the swollen polymer mass is similar in both gel-type and macroreticular resins (3a,b). Nanopores are actually formed by the void space surrounding the polymeric chains, as shown in level 4, and are a few nanometer wide. (Reprinted from Ref [12], 2003, with permission from Elsevier.)...
It has been previously reported [21, 22] that metal colloids are formed by radiochemical reactions in water/alcohol solutions, in which the reduction of metal salts takes place by solvated electrons and free radicals produced under UV or y-ray irradiation. Ichikawa et al. have applied this photoreduction method to the surface-mediated reaction of metallic ions and succeeded in synthesizing metal/aUoy nanowires in the constrained cavities of mesoporous supports such as FSM-16 and MCM-41 [18-20, 23-25]. The adsorbed water and alcohol work not only as solvents in the nanoscale silica void space but also as a source of reducing species for metallic ions to metals under UV-vis and y-ray [11, 18, 19] irradiation. The results indicate the dense formation of Pt nanowires inside the charmels of mesoporous supports, such as FSM-16, which act as the templates. In fact, no any Pt wire is observed on the external surface of FSM-16 or amorphous silica surface. Short wires, 10 nm long, are also observed as a minor species in the samples in the initial stage of UV and y-ray irradiation. [Pg.601]

As will be shown, model systems for cells employing lipids or composed of polymers have been in existence for some time. Model systems for coccolith-type structures are well known on the nanoscale in inorganic and materials chemistry. Indeed, many complex metal oxides crystallize into approximations of spherical networks. Often, though, the spherical motif interpenetrates other spheres making the formation of discrete spheres rare. Inorganic clusters such as quantum dots may appear as microscopic spheres, particularly when visualized by scanning electron microscopy, but they are not hollow, nor do they contain voids that would be of value as sites for molecular recognition. All these examples have the outward appearance of cells but not all function as capsules for host molecules. [Pg.91]

Fig. 4.11. Left (a) Optical microscope image of an OLED working at a luminance of 100 cd/m2 under water vapor atmosphere. Non-emitting dark spots can be seen clearly, (b) SEM image of the bubbles formed on the aluminum cathode in the dark spot area, (c) Correlation between dark spot growths (taken from the increase in diameter) and total current density [110]. Right (a) Shown here is the random pattern of carbonized areas on the surface of the cathode after operation, shown in wide field, (b) At higher resolution, the structure of one of these areas becomes more apparent, (c) and (d) show nanoscale views of carbonized areas with the extrusion of the polymer through the cathode and the resulting void underneath [111]. Fig. 4.11. Left (a) Optical microscope image of an OLED working at a luminance of 100 cd/m2 under water vapor atmosphere. Non-emitting dark spots can be seen clearly, (b) SEM image of the bubbles formed on the aluminum cathode in the dark spot area, (c) Correlation between dark spot growths (taken from the increase in diameter) and total current density [110]. Right (a) Shown here is the random pattern of carbonized areas on the surface of the cathode after operation, shown in wide field, (b) At higher resolution, the structure of one of these areas becomes more apparent, (c) and (d) show nanoscale views of carbonized areas with the extrusion of the polymer through the cathode and the resulting void underneath [111].
Fig. 15.13 shows a bonding map for silicon wafer bonding combinations of topography and spatial wavelength that fall below the traces will bond those above the traces will produce voids [101]. This and further work by Turner et al. have explored parameters for direct wafer bonding under clamped conditions [107], addressed wafer bow and etch pattern considerations [108], as well as nanoscale roughness considerations [101]. This work shows that... [Pg.453]

Naturally occurring nanomaterials exist in a variety of complex forms. In this chapter a short set of definitions will be stated for clarity. Nanocrystals are single crystals with sizes from a few nm up to about 100 nm. They may be aggregated into larger units with a wide spectrum of microstructures. Nanoparticles are units of minerals, mineraloids or solids smaller in size than 100 nm, and composed of aggregated nanocrystals, nanoclusters or other molecular units, and combinations of these. Nanoclusters are individual molecular units that have well-defined structure, but too small to be true crystals. Al and ZnsSs solution complexes are types of nanoclusters with sizes from sub nanometer to a few nm. Nanoporous materials are substances with pores or voids of nanoscale dimensions. These materials can be single crystals, such as zeolites or... [Pg.105]

Nanostructured noble metal films (ex Ag) with thicknesses of <10 nm support plasmon oscillations. Such films are quasi-continuous and consist of isolated islands each of nanoscale diameter. These structures could therefore be modeled as 2D nanoisland lattices or as 2D photonic lattices of voids separating the islands. Brief iodization of these films causes a controlled depletion of electron density leading to a gradual disappearance of plasmons and a progressive buildup of excitons and valence band structure of Agl. The decay of plasmons in Ag is apparently closely connected with the buildup of electron-hole pairs in Agl as found in our recent iodization experiments. [Pg.308]

The nanoscale materials considered in this chapter are solid materials with primary particles sizes ranging from 1 to 100 nm (10 to 1000 A), as defined in Chapter 1 of the first edition (1). Materials referred to as powders are simply classified through observation rough powder (1 mm to 40 p.m, optical microscope), fine powder (40 p,m to 1 p,m, optical microscope), and superfine powder (<1 p,m, only visible by electron microscope). The latter, superfine powder or nanoparticles, may correspond to the primary particle. These nanoparticles are usually in the form of smoke, combusted particulates, and dispersed primary particles. Some rough and fine powders may be composed of primary particles if the surface area is high. The microstructure of a pellet or powder is important, because the chemical reaction starts from the surface (favored for small crystals) and gas diffuses through the void channels. The morphology controls the reaction rate, which is one of the main concerns in this chapter. [Pg.498]

Nanoscale clusters of metals or voids, which may be formed with irradiation (cf. Bjo as, 2012 Dubinko, 2012), interacts with dislocations at their boundaries in addition to DLs and branches inside the crystal. The formation of such permanent dislocation inside the material may give it superior hardness and yield strength, because it is not easy to move such dislocations (Kittle, 1996). That is why irradiated material is hardened (cf. Dubinko et al., 2009). Interaction of the radiation-induced electron cloud with nearby defect site may occur under certain conditions, while synthesis of new chemical compounds is dependent on the TDs of the inorganic material. Such effect may help in development of new materials or deterioration of an efQdent material. [Pg.414]

One goal of nanoscience in general and in the field of nanoporous materials " in particular is to achieve control over the architecture of matter on the nanoscale (1-100 nm). Because porous materials are divided into the subgroups microporous (voids smaller than 2 nm). mesoporous (voids between 2-50 nm). and macroporous (voids larger than 50 nm), it becomes obvious that these materials are raw models for nanostructured matter. Three... [Pg.950]


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See also in sourсe #XX -- [ Pg.178 ]




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