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Equilibrium carrier distribution

The following discussion outlines the universal features and the distinctions between the bulk and nanoscale limits for these various pathways. Specifically, this section will emphasise the most recent advances in our understanding of relaxation and transport phenomena in semiconductors, as they pertain to photoinduced perturbations in the equilibrium carrier distribution. Under equilibrium conditions, the electron (n) and hole (p) carrier densities satisfy the relation (Sze, 1981)... [Pg.43]

Equilibrium carrier energy, relative to the center of a distribution of hopping site energies, in eV E Electric field, in V/cm... [Pg.795]

For the trial function 4> k) one can employ (instead of performing a complete variational calculation) the ansatz (9.71), where the constant in equation (9.71) cancels in expression (9.75). The equilibrium charge-carrier distribution/ [.E(fc)] may be written as... [Pg.344]

Fig. 5.113 Sketch of the dopant (A acceptor, D donor) and carrier distribution in a symmetrical pn-jimction in thermal equilibrium. Fig. 5.113 Sketch of the dopant (A acceptor, D donor) and carrier distribution in a symmetrical pn-jimction in thermal equilibrium.
The distributions of excess, or injected, carriers are indicated in band diagrams by so-called quasi-Fenni levels for electrons or holes (Afp). These functions describe steady state concentrations of excess carriers in the same fonn as the equilibrium concentration. In equilibrium we have... [Pg.2890]

The carrier-phonon interaction decreases with the lowering of temperature, since the emission and absorption of phonons by carriers is proportional to the number of final states available to carriers and phonons. At sufficiently low temperatures, the interaction between the two subsystems can be so weak that there is no thermal equilibrium between them, and the energy is distributed among electrons more rapidly than it is distributed to the lattice, resulting in a different temperature for electron and phonon subsystems, giving rise to the so-called electron-phonon decoupling . [Pg.327]

This group of ISEs is based on the ion-selective character of the distribution equilibrium between water and the membrane phase. As was demonstrated in chapter 3, this ion-selectivity may be affected if an ion pair is formed in the membrane (section 3.2) and increased markedly if complexes are formed in the membrane between the test ion and special complexing agents, ion carriers or ionophores (section 3.3). [Pg.174]

Let us consider the distribution of a trace element A and a carrier B between a crystal and an ideal aqueous solution at equilibrium. Defining... [Pg.659]

In an attempt to minimize the compositional effects of phases on trace partitioning, Henderson and Kracek (1927) also introduced the concept of normalized partition coefficient D, which compares the relative trace/carrier (Tr/Cr) mass distributions in the two phases at equilibrium—i.e.. [Pg.681]

Due to the ionic nature of cephalosporin molecules, the interfacial chemical reaction may in general be assumed to be much faster than the mass transfer rate in the carrier facilitated transport process. Furthermore, the rate controlling mass transfer steps can be assumed to be the transfer of cephalosporin anion or its complex, but not that of the carrier. The distribution of the solute anion at the F/M and M/R interfaces can provide the equilibrium relationship [36, 69]. The equilibrium may be presumably expressed by the distribution coefficients, mf and m at the F/M and M/R interfaces, respectively and these are defined as... [Pg.222]

Note also that p8 and ns, appearing in Eqs. (23) and (24), generally do not coincide with those given by equilibrium distributions (13), even in the absence of illumination. The electrode reaction can disturb significantly the distribution of charge carriers in a semiconductor electrode. In particular, if minority carriers become involved in an electrode reaction, its rate may be limited by the rate at which these carriers are supplied from the bulk of the semiconductor to its surface. [Pg.272]

It would lie far beyond the aim of this chapter to introduce the state-of-the art concepts that have been developed to quantify the influence of colloids on transport and reaction of chemicals in an aquifer. Instead, a few effects will be discussed on a purely qualitative level. In general, the presence of colloidal particles, like dissolved organic matter (DOM), enhances the transport of chemicals in groundwater. Figure 25.8 gives a conceptual view of the relevant interaction mechanisms of colloids in saturated porous media. A simple model consists of just three phases, the dissolved (aqueous) phase, the colloid (carrier) phase, and the solid matrix (stationary) phase. The distribution of a chemical between the phases can be, as first step, described by an equilibrium relation as introduced in Section 23.2 to discuss the effect of colloids on the fate of polychlorinated biphenyls (PCBs) in Lake Superior (see Table 23.5). [Pg.1174]


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See also in sourсe #XX -- [ Pg.2 ]




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Equilibrium distribution

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