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Absorption of electrons

We shall be dealing throughout this chapter with many situations in which various atomic solutes in a solid solution can react to form a variety of complexes, which in turn can redissociate into their atomic constituents. Some of these may exist in different charge states, which can interconvert by emission or absorption of electrons or holes. When the various atomic or electronic reactions have come to equilibrium, the concentrations of the various species involved will have to obey certain equilibrium relations. In this section, we shall review these in a language suitable for analysis of the various experiments to be discussed in Section III. [Pg.249]

A quite different aspect of local kinetics is that having to do with changes of charge state, e.g., between H+ and H° or H° and H. Such changes require emission or absorption of electrons or holes. Since the mean free paths of these carriers are large compared with atomic dimensions, it is customary (see for example Lax, 1960) to use a velocity-averaged cross section a as the key descriptor of the rate of a capture reaction such as H+ + e— H°. Explicitly, we write, for this case,... [Pg.255]

Timusk, T., and A. Silin, 1975. Far-infrared absorption of electron-hole drops in pure and doped germanium, Phys. Status Solidi (b), 69, 87-91. [Pg.517]

Fig. 1. Top Reference spectra for femtosecond transient absorption measurements S-S abs. in solution (thin solid lines), oxidized dye (dye+) abs. in solution (thick solid line), fluorescence for solution (dotted line), steady-state absorption ofNKX-2311/ZnO (dotted-dashed line), and absorption of electrons in the conduction band (dashed line). Bottom Transient absorption spectra of NKX-23ll/ZnO in the spectral range between 600 and 1350 nm at the 2 (thick solid line), 10 (dotted line), 100 ps (thin solid line) delay times after excitation at 540 nm by the femtosecond pulse with the intensity of about 10 pJ. Fig. 1. Top Reference spectra for femtosecond transient absorption measurements S-S abs. in solution (thin solid lines), oxidized dye (dye+) abs. in solution (thick solid line), fluorescence for solution (dotted line), steady-state absorption ofNKX-2311/ZnO (dotted-dashed line), and absorption of electrons in the conduction band (dashed line). Bottom Transient absorption spectra of NKX-23ll/ZnO in the spectral range between 600 and 1350 nm at the 2 (thick solid line), 10 (dotted line), 100 ps (thin solid line) delay times after excitation at 540 nm by the femtosecond pulse with the intensity of about 10 pJ.
This is a Pascal distribution with cascade process not only magnifies the average number of electrons, but also the fluctuations about that average. Later work took into account the absorption of electrons, their distribution over various energies, and the photons as a separate entity. 0... [Pg.146]

The absorption of electrons by a surface is measured as a function of energy and angle. This technique gives information about conduction bands and unoccupied levels. [Pg.519]

The contrast in the image is formed from the interactions between the incident electrons and the matter. The most common operating mode in TEM is the bright field imaging mode. In this mode and in the case of non crystalline materials such as polymers, the contrast is formed directly by absorption of electrons in the sample. Actually, the image is assumed to be a simple two dimensional projection... [Pg.53]

Sharata, H. and R. R. Burnette. Percutaneous absorption of electron-dense ions across normal and chemically perturbed skin. J. Pharm. Sci. 77 27-32 (1989). [Pg.213]

A very few highly diluted gases have, however, been the objects of coherent electron scattering experiments. In more dense gases, absorption of electrons rapidly becomes predominant and hinders measuring scattering intensities. Diffraction of electrons thus allowed determining with precision the structure of H-bonded cyclic dimers of carboxylic acids (26-28) that constitute model systems of H-bonds we have already seen in Ch. 2 and shall see later in this book. They nevertheless remain scarcely used methods. [Pg.66]

The Energy Rate Coefficients / Xk and Axk- Pxk, a rate coefficient analogous to aXK but specifying the rate of absorption of electron energy in effecting any particular Reaction, Rl, is given by... [Pg.469]

The strong electronic absorption of alkane radical cations is readily understood in molecular orbital terms. Extending down from the highest occupied molecular orbital (HOMO) is a rather closely packed set of valence molecular orbitals, that are clearly displayed in the photoelectron spectra (PES) of neutral alkanes. The electronic absorption of alkane radical cations is due to transitions (induced by photon absorption) of electrons from such lower-lying molecular orbitals to the semi-occupied molecular orbital (SOMO), which is the highest-occupied molecular orbital in the ground-state ion. By illumination within the (broad and largely unstructured) absorption band of alkane radical cations, electronically excited states of alkane radical cations can thus be created in a quite convenient way. [Pg.109]

In fact the transmission signal itself reflects the absorption of electrons in specimen. The information depth thus depends on the combination of specimen thickness (and composition) and applied high voltage. [Pg.79]

A series of reactions, such as splitting of the cations [Eq. (6.69)], absorption of electrons by cationic species [Eq. (6.70)] or neutral species [Eq. (6.71)] to form radicals or anions, respectively, and anion splitting to form radical [Eq. (6.72)] and radical plus electron [Eq, (6.73)], may then take place ... [Pg.340]

The electrochemical processes occurring in this cell are the oxidation of zinc and the production of zinc sulfate and electrons at the anode, the absorption of electrons an the reduction and deposition of copper at the cathode, the flow of electrons through an external electrical circuit (resulting in electrical work), and a balancing flow of sulfate ions through the salt bridge. [Pg.812]

Most of the sample molecules are not ionized at all but are continuously drawn off by vacuum pumps that are connected to the ionization chamber. Some of the molecules are converted to negative ions through the absorption of electrons. The repeller plate absorbs these negative ions. A small proportion of the positive ions that are formed may have a charge greater than one (a loss of more than one electron). These are accelerated in the same way as the singly charged positive ions. [Pg.391]

Other phenomena that can be exploited are, e.g., emission of photons (light) and absorption of electrons (Amelinckx et al. 1997). If the... [Pg.1088]


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See also in sourсe #XX -- [ Pg.58 ]




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