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HAMMOU, M. KLEITZ, E. SIEBERG, J-L. SOUQUET, Electrochimie des solides, Collection Grenoble Sciences, 1994. 2. M. SOUSTELLE, Modélisation macroscopique des transformations physico-chimiques, Masson, Paris, 1990. 3. A. , 1974. Physical Chemistry of Solid-Gas Interfaces: Concepts and Methodology for Gas Sensor Development Rene Lalauze Copyright 02008, ISTE Ltd. 1. Introduction Before going into a description of electron transfers between a gas and a solid, it is necessary to present some general physical or physico-chemical properties of the constituents, that is to say gases and solids.
SIEBERG, J-L. SOUQUET, Electrochimie des solides, Collection Grenoble Sciences, 1994. 2. M. SOUSTELLE, Modélisation macroscopique des transformations physico-chimiques, Masson, Paris, 1990. 3. A. , 1974. Physical Chemistry of Solid-Gas Interfaces: Concepts and Methodology for Gas Sensor Development Rene Lalauze Copyright 02008, ISTE Ltd. 1. Introduction Before going into a description of electron transfers between a gas and a solid, it is necessary to present some general physical or physico-chemical properties of the constituents, that is to say gases and solids.
In our case, there is only one particle and we hope to achieve a near-zero value for the probability on the entire space domain, except a very small area around the particle. This result cannot be obtained mathematically unless the Mg function wave vectors are slightly different, which boils down to an interference problem. As an example, we can easily deal with the case of the function: Mg M 0 sin> k 0 g'k x @ The wave vector kg varies from: k0 = ' k to k0 + N'k when g ranges from 1 to N. 3a.