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Charge generation diffusion charging

As time progresses, charge is generated by photon currents, semiconductor dark currents, diffusion, depletion, surface, avalanche, and tunneling. The time required to fill the well by dark currents is the storage time, given by the following. [Pg.425]

Figure 7. Adsorption of an electronegative species from the gas phase onto a metal surface generates a dipolar layer due to electron transfer from the metal to the species. Adsorption of anions onto an electrode simulates the situation when the positive charge on the metal compensates for the adsorbed negative charge (zero diffuse-layer charge), and not when the charge on the metal is zero. Figure 7. Adsorption of an electronegative species from the gas phase onto a metal surface generates a dipolar layer due to electron transfer from the metal to the species. Adsorption of anions onto an electrode simulates the situation when the positive charge on the metal compensates for the adsorbed negative charge (zero diffuse-layer charge), and not when the charge on the metal is zero.
The Gartner model simulates charge collection by a potential-dependent space charge layer and considers diffusion into the space charge layer of charge carriers generated deep inside the semiconductor. The well-known Gartner formula for the photocurrent /ph is... [Pg.467]

The same property of entropy generation holds for other processes. In electrical conductance, charged particles move from higher to lower electrical potentials. In diffusion phenomena, all chemical entities are transferred from higher to lower chemical potentials. [Pg.119]

Fig. 8 Long range charge transport between dppz complexes of Ru(III) and an artificial base, methyl indole, in DNA. The methyl indole is paired opposite cytosine and separated from the intercalating oxidant by distances up to 37 A. In all assemblies, the rate constant for methyl indole formation was found to be coincident with the diffusion-controlled generation of Ru(III) (> 107 s )> indicating that charge transport is not rate limiting over this distance regime... Fig. 8 Long range charge transport between dppz complexes of Ru(III) and an artificial base, methyl indole, in DNA. The methyl indole is paired opposite cytosine and separated from the intercalating oxidant by distances up to 37 A. In all assemblies, the rate constant for methyl indole formation was found to be coincident with the diffusion-controlled generation of Ru(III) (> 107 s )> indicating that charge transport is not rate limiting over this distance regime...

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See also in sourсe #XX -- [ Pg.115 , Pg.116 ]




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Diffusivity 208 - generation

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