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Substrate-induced charging

V (y) is the reverse bias applied in the perpendicular direction to the field-effect induced p-n junction created by the n-type surface inversion layer and the p-type substrate. The charge 2b (y) created by the immobile ionized atoms of the dopant forms the space charge region. The depletion approximation assumes that there are no mobile charges at all in the space charge regions. Under that assumption, (C.24) applies. [Pg.362]

The application of semiconductors as substrates in interfacial supramolecular assemblies has been dominated so far by films consisting of nanoparticles. In an attempt to understand the properties of such particles, and in particular, issues such as light-induced charge separation, their electronic properties will be discussed in some detail. Relevant issues in this respect are quantum effects, the size of the band gap, charge transport and band bending. [Pg.266]

The method uses a silver hydrosol active substrate. A charge-coupled device was used as the detector. All measurements were made with a 180° scattering geometry. The 507.1 nm line of an Ar-ion in laser (Spectra-Physics Model 2020) was used for excitation with a laser power of 6-8 mW at a resolution of 2 cm-1. Prior to inducing the SERRS effect, the nitrite was transformed into a colored azo dye. [Pg.345]

The WOC is oxidized stepwise by a nearby tyrosine residue (Tyrz), which is itself oxidized by the chlorophyll cation radical P680+ (formed by light-induced charge separation). The electrons are eventually used by PSII for the reduction of plastoqui-none. After the WOC has lost four electrons, the accumulated oxidizing power drives the formation of molecular oxygen from two substrate water molecules, and the catalytic system is reset. The sequence of the four electron-transfer steps is summarized in the Kok cycle [32] of Figure 4.5.3, where the most probable spectroscopically derived oxidation states of the Mn ions [33] are shown for each of the five redox state intermediates S (n - 0-4). [Pg.362]

Absorption peaks at 0.55 eV and 1.01 eV are also found by Harrison et al. (sec results on field induced charges) and attributed to 7t-dimers in highly ordered films. Because Oeter et al. did not study the geometric structure of their films, this interpretation has not been proved so far, although in thick films intermixed with FeCli on Au substrates a highly disordered film is expected. [Pg.714]

The incommensurate, hexagonal monolayers are compressed compared to the bulk metal and they are rotated from the substrate by several degrees. From the results, the monolayer compressibility could be calculated. The restructuring (i.e. surface reconstruction) of top layers of single crystal metal surfaces as a function of solution composition and electrode potential has been studied [73]. The induced charge density was found to be the critical parameter [74]. Structural changes during... [Pg.244]

An ion in solution has a repulsive interaction from the surface when the solution dielectric constant is higher than that of the substrate. This effect can lead to desorption for highly charged PE chains. On the contrary, when the substrate is a metal, there is a possibility to induce PE adsorption on noncharged substrates or on substrates bearing charges of the same sign as the PE. See Ref. [84] for more details. [Pg.300]


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