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Semiconductor chemisorption functions

Having established the expressions for the chemisorption functions of an AB-type chain, we can now employ them in calculating AE (4.101) and Aq (4.102) for oxygen on narrow-gap III-V semiconductors. Specifically, we are interested in GaSb, InAs and InSb. The choice of narrow-gap substrates ensures that the approximation made regarding the contour C in (4.92) remains valid. Results are presented for the 47-case only. [Pg.74]

The change in the work function and the electrical conductivity of the semiconductor due to chemisorption is the second important consequence of the theory. These effects have been theoretically considered in detail by Sandomirsky 46-48) They have been observed experimentally by a number of authors 49-64)- Some of the experimental data are presented in Table I, where the signs -f- and — denote, respectively, positive and negative surface charging upon chemisorption (Ao- > 0 or Ac < 0) these data have been obtained from the variation of the work function or of the electrical conductivity or both simultaneously. The symbol x in the table denotes that the surface charge is not affected by chemisorption (Ao- = 0) the figures in brackets refer to the literature. [Pg.234]

Chemisorption leads to a change in the work function and the electrical conductivity of the semiconductor (Sec. VI,C). This is caused by charging of the surface in chemisorption, which fact is in turn a result of the existence of the strong forms of chemisorption. [Pg.260]

In the preceding chapters the conditions determining chemisorption and the thermodynamic treatment of surface equilibria have been discussed. We shall now derive a general formula for the dependence of the work function of a semiconductor (e.g. of an oxide) upon the surface concentration of the chemisorbed oxygen ions. [Pg.230]

In the preceding chapter we pointed to electrical conductivity as one of the physical properties of semiconductors which is changed by a chemisorption process and is accessable to measurement. A further possibility for investigating the mechanism of chemisorption is the relation between the work function and the external electric field of the semiconductor as influenced by chemisorption. These effects have been used for the interpretation of the mechanism of chemisorption and heterogeneous catalysis by Suhrmann (42), and have been experimentally demonstrated in chemisorption processes by Ljaschenko and Stepko. These effects shall here be correlated with our concept of the boundary layer formed in the presence of oxygen and hydrogen. [Pg.230]

If we first consider only those chemisorption processes in which an electron transfer takes place from the semiconductor to the chemisorbing gas, we can summarize the result of these calculations as follows The value of the work function must increase if a chemisorption takes place with the consumption of electrons by the chemisorbed gas. The increase of the work function can be expressed in the case of an w-conducting adsorbent by a quadratic, and in the case of a p-conducting adsorbent by a combined linear-logarithmic dependence on the surface concentration of the... [Pg.231]

Keywords Chemisorption surface structure cycloaddition silicon dimer semiconductor functionalization 7r bonding free-radical reactions. [Pg.333]

Interactions at room temperature When CO is first introduced (Fig.l), a increases irtfantaneously and then remains independent of P 0. The fact that a does not decrease means that CO does not dissociate on titania nor at the interface, otherwise the filling of anionic vacancies by atomic oxygen (Eq,-6) would have decreased substantially a by consuming free electrons. The sharp initial increase, on the contrary, shows that CO chemisorb on Pt with a donor effect probably due to the creation of dipoles as proposed for H. chemisorption which renders ohmic the electrical contact between the metal and its semiconductor support (26, 17, 28)Accordlng to these authors, the creation of a dipole layer decreases the work function of the metal which approaches the electron affinity of the semiconductor, thus suppressing the Schottky barrier. Presently CO adsorbs as a donor molecule on Pt decreasing 0, which allows elec-... [Pg.203]

Figure 20-24 shows the resistance of Zr02-MgO as a function of water vapor content (ppmw). The resistance decreases rapidly with an increase in water vapor from 10 to 10 ppmw. Compared with the ionic-type humidity sensor, the response of the semiconductor-type is rather slow because of the slow rate of chemisorption or the subsequent electron transfer process on the oxide surface. The microstructure of the elements as defined by surface area and average particle size, has a less pronounced effect on sensing characteristics than is the case in the ionic-type humidity sensors [31]. [Pg.299]

Similar considerations apply in the case of donor states introduced by electropositive gases. In this case, an electron is transferred from the approaching molecule to the semiconductor. The energy of chemisorption is W< -1, where I is the ionization energy of the adsorbate. In this situation, adsorption of an electropositive molecule leads to a downward bending of the energy band and a reduction in the work function (Many et al. 1965). [Pg.247]

Selzer and Cahen [128] showed that a complementary configuration can be used, as well. They adsorbed ligands on the metal rather than on the semiconductor side of the junction. In that case the metal work function, rather than the semiconductor s electron affinity is changed. They used the molecules of Ref. [8], which are similar to those shown in Fig. 7(a), but with cyclic disulfide, instead of dicar-boxylic acid binding groups, so as to allow chemisorption onto Au. The molecularly modified metal was then used to prepare Au/molecule/SiOx/Si diodes. Results are naturally opposite to those obtained with GaAS/Au diodes [77], because the substituted phenyl groups point in opposite directions in the two cases. [Pg.144]

Concludig the discussion of hybrid functionals we stress that the HSE functional is universally apphcable and does not contain any system-dependent parameter. It yields excellent results, in molecules and solids, for many different properties. In contrast to other methods, HSE can be employed for both structural and electronic properties HSE provides a unique and powerful alternative for the study of large complex systems, such as chemisorption at surfaces and three-dimensional impurities in semiconductors. These fields of HSE functional applications await future study. [Pg.269]

Tin pyrophosphate (SnP207) was synthesised and tested as an anode in lithium ion batteries. P MAS NMR indicates a single species near in position to that expected for Li3P04 but this species would be inconsistent with the observed phosphate reduction. Li MAS NMR shows no presence of Li20. To advance the work on the characterisation of Ti02 hetero-assemblies formed by surface modification with functional molecular materials, solid-state NMR study was carried out on the molecules chemisorption on the surface of the semiconductor by P solid-state NMR. ... [Pg.324]


See other pages where Semiconductor chemisorption functions is mentioned: [Pg.12]    [Pg.13]    [Pg.55]    [Pg.223]    [Pg.30]    [Pg.55]    [Pg.57]    [Pg.333]    [Pg.351]    [Pg.78]    [Pg.762]    [Pg.26]    [Pg.482]    [Pg.7]    [Pg.180]    [Pg.818]    [Pg.247]    [Pg.317]    [Pg.108]    [Pg.699]    [Pg.16]    [Pg.358]   
See also in sourсe #XX -- [ Pg.69 ]




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