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Silver particles

Kriebig U and Fragstein C V 1969 The limitation of electron mean free path in small silver particles Z. Physik 224 307... [Pg.2922]

Polymer thick films also perform conductor, resistor, and dielectric functions, but here the polymeric resias remain an iategral part after cuting. Owiag to the relatively low (120—165°C) processiag temperatures, both plastic and ceramic substrates can be used, lea ding to overall low costs ia materials and fabrication. A common conductive composition for flexible membrane switches ia touch keyboards uses fine silver particles ia a thermoplastic or thermoset polymeric biader. [Pg.126]

He studied the sintering of copper particles in the diameter range 15-100 microns and of silver particles of diameter 350 microns. The results for the larger volume fraction of copper and for silver were shown to fit the volume diffusion mechanism and yielded the results for volume self-diffusion... [Pg.206]

The results for silver particles show the way in which die average particle size of the spheres modifies the map of the predominating mechanisms which depend on the sphere diameter, a, in differing ways as shown above in the variation in the values of m which can be shown in the form of a general equation... [Pg.207]

Much care had to be taken during the TEM observations of silver nitrate filled tubes, because this salt is very sensitive to electron irradiation and the continuous filaments transformed quickly into a chain of silver particles (see Fig. 5) [22]. [Pg.135]

Fig. 5. HREM of enclosed silver particles in CNTs. The metallic particles were obtained by electron irradiation-induced decomposition of introduced silver nitrate. Note that the gases produced by the nitrate decomposition have eroded the innermost layer of the tube. Fig. 5. HREM of enclosed silver particles in CNTs. The metallic particles were obtained by electron irradiation-induced decomposition of introduced silver nitrate. Note that the gases produced by the nitrate decomposition have eroded the innermost layer of the tube.
Figure 5.43. UP-spectra of Ag YSZ electrodes for (a) cathodic and (b) anodic polarization of the galvanic cell Ag YSZ Pd,PdO at 547°C. In (b), the shift of the Fermi edge of the small silver particles on YSZ under anodic polarization is shown enlarged (5x).24 Reprinted with permission from Wiley-VCH. Figure 5.43. UP-spectra of Ag YSZ electrodes for (a) cathodic and (b) anodic polarization of the galvanic cell Ag YSZ Pd,PdO at 547°C. In (b), the shift of the Fermi edge of the small silver particles on YSZ under anodic polarization is shown enlarged (5x).24 Reprinted with permission from Wiley-VCH.
Ozin and Huber 112) synthesized and characterized very small silver particles, Ag n = 2-5) by conventional deposition methods, as well as by a novel technique that they have termed "cryophotoaggrega-tion. This study will be discussed in detail in Section III. Of interest here is a study of silver atoms and small, silver clusters entrapped in ice and high-molecular-weight paraffin (n-C22H46, n-C32Hg8) matrices 146) (see Figs. 7 and 8, and Tables IV and V). Besides the intriguing, multiple-site (solvation) occupancy of atomic silver in ice matrices, and their thermal and photochemical interconvertibility, their extremely... [Pg.93]

FIG. 10 (a)n-A isotherms for oleic acid-capped silver particles the labels refer to the different phases as described in the text, (b) BAM micrographs at surface areas of (a) 5000-nm particle (b) 3200-nm particle during compression, (c) 1500-nm particle during compression, and (d) 5000-nm particle after re-expansion. The scale bar represents 1 mm. The micrographs are identified by the letters in the upper left corner of each image. (Reprinted with permission from Ref. 111. Copyright 1996 American Chemical Society.)... [Pg.75]

BAM showed bright regions due to the Ag particles and dark regions occupied primarily by oleic acid (Fig. 10b). TEM showed monolayer domains of surfactant-coated silver particles within regions of oleic acid. Vertical transfer onto quartz plates of up to eight layers with good linearity was reported. [Pg.76]

The production of fatty acid-capped silver nanoparticles by a heating method has been reported [115]. Heating of the silver salts of fatty acids (tetradecanoic, stearic, and oleic) under a nitrogen atmosphere at 250°C resulted in the formation of 5-20-nm-diameter silver particles. Monolayers of the capped particles were spread from toluene and transferred onto TEM grids. An ordered two-dimensional array of particles was observed. The oleic acid-capped particle arrays had some void regions not present for the other two fatty acids. [Pg.76]

FIG. 11 TEM images of 2.8-nm-diameter silver particles capped by dodecanethiol that were horizontally transferred from the water surface at a surface pressure just below that at which the film would collapse. The top figure is a higher-resolution image of this phase of particles. (Reprinted with permission from Ref. 121. Copyright 1997 American Chemical Society.)... [Pg.78]

FIG. 12 TEM micrographs of wirelike assemblies of silver nanoparticles, (a) Octanethiol-capped silver nanoparticles of average diameter 3.4 nm deposited from hexane solution, (b) The same particles deposited from heptane solution, (c) Octanethiol-capped silver particles of average diameter 4.4 nm deposited from heptane solution. (Reproduced with permission from Ref. 130. Copyright 1998 American Chemical Society.)... [Pg.80]

The formation of semiconductor nanoparticles and related stmctures exhibiting quantum confinement within LB films has been pmsued vigorously. In 1986, the use of the metal ions in LB films as reactants for the synthesis of nanoscale phases of materials was described [167]. Silver particles, 1-2 mn in size, were produced by the treatment of silver be-henate LB films with hydrazine vapor. The reaction of LB films of metal salts (Cd, Ag, Cu, Zn, Ni, and Pb ) of behenic acid with H2S was mentioned. The use of HCl, HBr, or HI was noted as a route to metal halide particles. In 1988, nanoparticles of CdS in the Q-state size range (below 5 mn) were prepared inside LB films of cadmium arachi-... [Pg.89]

When the silver nanocrystals are organized in a 2D superlattice, the plasmon peak is shifted toward an energy lower than that obtained in solution (Fig. 6). The covered support is washed with hexane, and the nanoparticles are dispersed again in the solvent. The absorption spectrum of the latter solution is similar to that used to cover the support (free particles in hexane). This clearly indicates that the shift in the absorption spectrum of nanosized silver particles is due to their self-organization on the support. The bandwidth of the plasmon peak (1.3 eV) obtained after deposition is larger than that in solution (0.9 eV). This can be attributed to a change in the dielectric constant of the composite medium. Similar behavior is observed for various nanocrystal sizes (from 3 to 8 nm). [Pg.321]

FIG. 5 Absorption spectra of coated silver particles dispersed in hexane and considered as isolated Average particle size 4 nm (A) and 5 nm (B). The dashed lines (b) are the Lorentzian simulations of the absorption spectra (a). [Pg.322]

When silver particles are self-organized in a 2D superlattice on Au(lll) substrate (Fig. IB), the recorded I(V) curve is that given in Figure 9B. For large biases, the detected current is reduced by more than one order of magnitude compared to that observed for isolated particles. This indicates an increase in the ohmic contribution to the current. The... [Pg.325]

Let us come back to the sample preparation A drop of solution containing silver nanoparticles dispersed in hexane is deposited on the substrate. The nanocrystals can be removed by washing the substrate and collected in hexane. The absorption spectrum of silver particles recorded before and after deposition remains the same. This indicates that coalescence does not take place. Similar behavior was observed by using HOPG as a substrate [6,35]. [Pg.327]


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See also in sourсe #XX -- [ Pg.521 , Pg.522 ]

See also in sourсe #XX -- [ Pg.624 ]




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