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Electrolyte junction

Figure 27. Minority charge carrier profiles near the semiconductor/electrolyte junction. calculated for a silicon interface at two different electrode potentials. Uf- -0.25 V and Uf= 5.0 V10 ((//= forward bias = t/ - Ufl>). Figure 27. Minority charge carrier profiles near the semiconductor/electrolyte junction. calculated for a silicon interface at two different electrode potentials. Uf- -0.25 V and Uf= 5.0 V10 ((//= forward bias = t/ - Ufl>).
Following the same procedure, the kinetic constants have been determined for very different electrochemical conditions. When n-WSe2 electrodes are compared in contact with different redox systems it is, for example, found9 that no PMC peak is measured in the presence of 0.1 M KI, but a clear peak occurs in presence of 0.1 M K4[Fe(CN)6], which is known to be a less efficient electron donor for this electrode in liquid junction solar cells. When K4[Fe(CN)6] is replaced by K3[Fe(CN)6], its oxidized form, a large shoulder is found, indicating that minority carriers cannot react efficiently at the semiconductor/electrolyte junction (Fig. 31). [Pg.487]

Control of Interfacial Lifetime in Silicon with Polymer/Electrolyte Junction... [Pg.497]

The PMC transient-potential diagrams and the equations derived for PMC transients clearly show that bending of an energy band significantly influences the charge carrier lifetime in semiconductor/electrolyte junctions and that an accurate interpretation of the kinetic meaning of such transients is only possible when the band bending is known and controlled. [Pg.503]

How can such problems be counterbalanced Since a large capacitance of a semiconductor/electrolyte junction will not negatively affect the PMC transient measurement, a large area electrode (nanostructured materials) should be selected to decrease the effective excess charge carrier concentration (excess carriers per surface area) in the interface. PMC transient measurements have been performed at a sensitized nanostructured Ti02 liquidjunction solar cell.40 With a 10-ns laser pulse excitation, only the slow decay processes can be studied. The very fast rise time cannot be resolved, but this should be the aim of picosecond studies. Such experiments are being prepared in our laboratory, but using nanostructured... [Pg.505]

Polymer-electrolyte junctions, lifetimes of carriers with, 496... [Pg.638]

Tacconi NR, Chenthamarakshan CR, Rajeshwar K, Tacconi El (2005) Selenium-modified titanium dioxide photochemical diode/electrolyte junctions Photocatalytic and electrochemical preparation, characterization, and model simulations. 1 Phys Chem B 109 11953-11960... [Pg.203]

Fig. 5.16 Energy-level diagram of p-CuInSe2/electrolyte junction. (Reprinted from [306], Copyright 2009, with permission from Elsevier)... Fig. 5.16 Energy-level diagram of p-CuInSe2/electrolyte junction. (Reprinted from [306], Copyright 2009, with permission from Elsevier)...
Aruchamy A, Wrighton MS (1980) Comparison of the interface energetics for n-type cadmium sulfide/ and cadmium teUuride/nonaqueous electrolyte junctions. J Phys Chem 84 2848-2854... [Pg.295]

Lemasson P, Etcheberry A, Gautron J (1982) Analysis of photocurrents at the semiconductor-electrolyte junction. Electrochim Acta 27 607-614... [Pg.297]

Lemasson P, Boutry AE, Tiiboulet R (1984) The semiconductor-electrolyte junction Physical parameters determination by photocurrent measurement throughout the Cdi xZnxTe alloy series. J Appl Phys 55 592-594... [Pg.298]

Energy level diagram of a semiconductor-electrolyte junction and solid-state and electrochemical energy scales. [Pg.230]

The different types of quinones active in photosynthesis are being used as electron acceptors in solar cells. The compounds such as Fd and NADP could also be used as electron/proton acceptors in the photoelectrochemical cells. Several researchers have attempted the same approach with a combination of two or more solid-state junctions or semiconductor-electrolyte junctions using bulk materials and powders. Here, the semiconductors can be chosen to carry out either oxygen- or hydrogen-evolving photocatalysis based on the semiconductor electronic band structure. [Pg.264]

This section and the next are dedicated to the basics of the silicon-electrolyte contact with focus on the electrolyte side of the junction and the electrochemical reactions accompanying charge transfer. The current across a semiconductor-electrolyte junction may be limited by the mass transport in the electrolyte, by the kinetics of the chemical reaction at the interface, or by the charge supply from the electrode. The mass transport in the bulk of the electrolyte again depends on convection as well as diffusion. In a thin electrolyte layer of about a micrometer close to the electrode surface, diffusion becomes dominant The stoichiometry of the basic reactions at the silicon electrode will be presented first, followed by a detailed discussion of the reaction pathways as shown in Figs. 4.1-4.4. [Pg.51]


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See also in sourсe #XX -- [ Pg.304 ]




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