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Metal particles, chemical principles

In principle, it should be possible to obtain experimental valence band spectra of highly dispersed metals by photoemission. In practice, such spectra is difficult to obtain because very highly dispersed metals are usually obtained only on nonconductive supports and the resulting charging of the sample causes large chemical shifts and severe broadening of the photoelectron spectra. The purpose of this section is to discuss valence band and core level spectra of highly dispersed metal particles. [Pg.78]

The transformation of one substance into another was a matter of rearrangement of the particles. In principle this would permit the transformation of one metal into another just as properly as any other more familiar chemical change. Indeed it might be said it permitted the transformation of anything into anything else, and Boyle at one time claimed to have converted a little gold into silver, a claim only a rich man might feel free to make. ... [Pg.47]

The structure and stability of small gold particles is a function of the chemical and physical nature of the support on which they reside.7,116,151>152 Jt is clear that the extent of the influence of the support on a metal particle will depend on the fraction of the metal atoms directly in contact with it for particles of the same shape this will increase as the size decreases, but it will also depend on the shape of the particle, which is conditioned by the chemical forces at the interface. In principle the particle shape is determined by the contact angle 0 defined by the equation... [Pg.59]

This principle appears amenable to generalization active sites and catalyst promoters can be positioned in the same cage in order to systematically study catalyst promoter effects due to direct interaction of metal particles and metal ions. Quantum chemical calculations by van Santen et al. have resulted in detailed predictions, e.g., of the effects of Mg ions, that are in direct contact with zeolite-encaged Ir4 tetrahedra, on the adsorption of H2 (i72) or CO 373) on these clusters. These theoretical results should be verified experimentally, as they could form a basis for general predictions on the action of ionic promoters on chemisorbing transition metals. [Pg.209]

This review begins with the more complex methods and moves on to the simpler ones. In this context, complexity is defined as the number of species involved before finally obtaining the highly dispersed metal particles. Table I summarizes the principal features of the different methods used to prepare the metal particles on a support, which is the common feature of all the methods and thus is not included in the table. They are subdivided into groups when the principles are similar. We could have ordered the preparation methods differently, for instance, using a chemical approach starting from the oxidation state and nuclearity of the metal in the precursor compound, but this would not have served our purpose, specifically, to show the parameters that can possibly influence the behavior of the final metallic state. [Pg.60]

Table 1 summarizes some microstructural and electrochemical properties of porous Si anode materials, as pertaining to the second approach mentioned above, collected from the literature published since 2005. Several synthesis methods have been identified for preparing the porous Si anode materials (column 1, Table 1). One of the two most adopted methods is known as the metal-assisted chemical etching (MACE denoted as E in Table 1). The fundamental principle of this method can be found in the handbook chapter Porous Silicon Formation by Metal Nanoparticle Assisted Etching. Figure 2 shows an example of the MACE-derived porous Si particle. The other most adopted method is magnesiothermic reduction (denoted as M in Table 1). In this method (see handbook chapter Porous Silicon Formation by Porous Silica Reduction ), porous Si oxide materials are reduced by magnesium vapor under high-temperature thermal treatment. The porous Si oxide precursors may be synthesized via the conventional sol-gel processes. Porous Si particles with unique pore structures, such as hollow interior and ordered mesoporosity, may be obtained from Si oxides having the same pore structures which are achieved by using proper templates. Table 1 summarizes some microstructural and electrochemical properties of porous Si anode materials, as pertaining to the second approach mentioned above, collected from the literature published since 2005. Several synthesis methods have been identified for preparing the porous Si anode materials (column 1, Table 1). One of the two most adopted methods is known as the metal-assisted chemical etching (MACE denoted as E in Table 1). The fundamental principle of this method can be found in the handbook chapter Porous Silicon Formation by Metal Nanoparticle Assisted Etching. Figure 2 shows an example of the MACE-derived porous Si particle. The other most adopted method is magnesiothermic reduction (denoted as M in Table 1). In this method (see handbook chapter Porous Silicon Formation by Porous Silica Reduction ), porous Si oxide materials are reduced by magnesium vapor under high-temperature thermal treatment. The porous Si oxide precursors may be synthesized via the conventional sol-gel processes. Porous Si particles with unique pore structures, such as hollow interior and ordered mesoporosity, may be obtained from Si oxides having the same pore structures which are achieved by using proper templates.
While implementation of RDE is relatively simple, understanding the principles of RDE is difficult. The concepts are widely distributed in the optics and chemical physics literature, often described in terms difficult to imderstand by biophysical scientists. In this volume we have presented chapters from the experts who have studied metal particle optics and fluorophore-metal interactions. We believe this collection describes the fundamental principles for the widespread use of radiative decay engineering in the biological sciences and nanotechnology. [Pg.466]

Application of Chemical Principles in the Solution Synthesis and Processing of Ceramic and Metal Particles... [Pg.82]

After all, even in the first case we deal with the interaction of an electron belonging to the gas particle with all the electrons of the crystal. However, this formulation of the problem already represents a second step in the successive approximations of the surface interaction. It seems that this more or less exact formulation will have to be considered until the theoretical methods are available to describe the behavior both of the polyatomic molecules and the metal crystal separately, starting from the first principles. In other words, a crude model of the metal, as described earlier, constructed without taking into account the chemical reactivity of the surface, would be in this general approach (in the contemporary state of matter) combined with a relatively precise model of the polyatomic molecule (the adequacy of which has been proved in the reactivity calculations of the homogeneous reactions). [Pg.53]


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