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Valence energy

Table 11.8 Total energy (valence only) (+76 a.u.) as a function of basis set and electron correlation... Table 11.8 Total energy (valence only) (+76 a.u.) as a function of basis set and electron correlation...
These reactions show sulfur in the role of an oxidizing agent. The properties of compounds such as ZnS suggest they contain the sulfide ion, S-2. The formation of this ion again can be expected on the basis of the fact that the neutral sulfur atom has two electrons less than enough to fill the valence orbitals. Acquisition of two electrons completely fills the low energy valence orbitals and solid ionic compounds can be formed. [Pg.369]

Chlorine would have to lose seven electrons to reach an electron configuration like that of neon. But if it gained one, it would have the same stable electron configuration as argon. So that is what chlorine does. If it meets an atom with a high-energy valence electron, such as sodium, the electron migrates to the chlorine atom and forms a chloride ion ... [Pg.83]

Within the approximation that the valence electronic states can be described adequately as combinations of the above valence CSFs, the three JE, JE, and CSFs must be combined to form the three lowest energy valence electronic states of E symmetry. For the homonuclear case, the E CSF does not couple with the other two because it is of ungerade symmetry, while the other CSFs JE and1E have gerade symmetry and do combine. [Pg.232]

ESCA involves the measurement of binding energies of electrons ejected by interactions of a molecule with a monoenergetic beam of soft X-rays. For a variety of reasons the most commonly employed X-ray sources are Al and MgKol>2 with corresponding photon energies of 1486.6 eV and 1253.7 eV respectively. In principle all electrons, from the core to the valence levels can be studied and in this respect the technique differs from UV photoelectron spectroscopy (UPS) in which only the lower energy valence levels can be studied. The basic processes involved in ESCA are shown in Fig. 1. [Pg.127]

Figure 28.1 The electronic structure of a solid can be described in terms of a band model in which bonding electrons are primarily found in a low-energy valence band, while conduction is typically associated with antibonding or nonbonding high-energy orbitals known as the conduction band. In the case of a semiconductor (left), these two bands are separated by a quantum-mechanical forbidden zone, the band gap. Excitation of electrons from the valence band to the conduction band gives rise to the bulk optical and electronic properties of the semiconductor. In the case of a metal (right), the conduction band and valence band overlap, giving rise to a continuum of states. Figure 28.1 The electronic structure of a solid can be described in terms of a band model in which bonding electrons are primarily found in a low-energy valence band, while conduction is typically associated with antibonding or nonbonding high-energy orbitals known as the conduction band. In the case of a semiconductor (left), these two bands are separated by a quantum-mechanical forbidden zone, the band gap. Excitation of electrons from the valence band to the conduction band gives rise to the bulk optical and electronic properties of the semiconductor. In the case of a metal (right), the conduction band and valence band overlap, giving rise to a continuum of states.
Exercise 14-6 a. Write the initiation and propagation steps involved in the radical bromination of methylbenzene (toluene) with bromine. Write the low-energy valence-bond structures of the intermediate phenylmethyl radical. [Pg.547]

Why does the octet rule work What factors determine whether an atom is likely to gain or to lose electrons Clearly, electrons are most likely to be lost if they are held loosely in the first place—that is, if they feel a relatively low effective nuclear charge, Zeff, and therefore have small ionization energies. Valence-shell electrons in the group 1A, 2A, and 3A metals, for example, are shielded from the nucleus by core electrons. They feel a low Zeff, and they are therefore lost relatively easily. Once the next lower noble gas configuration is reached, though, loss of an additional electron is much more difficult because it must come from an inner shell where it feels a high Zeff. [Pg.230]

In electron correlation treatments, it is a common procedure to divide the orbital space into various subspaces orbitals with large binding energy (core), occupied orbitals with low-binding energy (valence), and unoccupied orbitals (virtual). One of the reasons for this subdivision is the possibility to freeze the core (i.e., to restrict excitations to the valence and virtual spaces). Consequently, all determinants in a configuration interaction (Cl) expansion share a set of frozen-core orbitals. For this approximation to be valid, one has to assume that excitation energies are not affected by correlation contributions of the inner shells. It is then sufficient to describe the interaction between core and valence electrons by some kind of mean-field expression. [Pg.127]

Edge energies, valence DR and dispersion of vanadium surface species... [Pg.181]

A further factor that has a marked influence upon the arene oxide-oxepin distribution is the effect of substituents. With the numbering system shown below, arene oxides, monosubstituted arene 1,2-, or 3,4-, and 1,2 disubstituted 1,2-oxides prefer their oxepin forms whereas arene 2,3-oxides prefer their oxide tautomers. These observations concur with MINDO/3 calculations and may be rationalized in terms of the maximum number of low-energy valence-bond structures for tt-electron-donating or withdrawing substituents (Figure 1). [Pg.200]

On this basis, if the highest filled core orbitals have opposite parity to the lowest energy valence shell orbitals, then the dominant component of the polarisation will be dipolar, leading to an accumulation of negative charge in... [Pg.266]

Electronic transitions within the valence shell of atoms and molecules appear in the energy-loss spectrum from a few electron volts up to, and somewhat beyond, the first ionization energy. Valence-shell electron spectroscopy employs incident electron energies from the threshold required for excitation up to many kiloelectron volts. The energy resolution is usually sufficient to observe vibrational structure within the Franck-Condon envelope of an electronic transition. The sample in valence-shell electron energy-loss spectroscopy is most often in the gas phase at a sufficiently low pressure to avoid multiple scattering of the... [Pg.1322]

This molecular excitation results in the generation of mobile electrons in the higher energy conduction band ( < /,) and positive holes in the lower energy valence band ( ,, ) of the catalyst, according to equation 1-1 and the reaction illustrated in Figure 1.1. [Pg.2]

Bonding electron energy, valence UV/VIS spectroscopy 180-800nm... [Pg.68]

Fig. 6.9 Space-charge region at a semiconductor surface, here represented for the case of an n-type semiconductor. Energy band profiles and electron concentration n(x). Ec, Ev, Ef respectively stand for conduction band energy, valence band... Fig. 6.9 Space-charge region at a semiconductor surface, here represented for the case of an n-type semiconductor. Energy band profiles and electron concentration n(x). Ec, Ev, Ef respectively stand for conduction band energy, valence band...
Ultraviolet photoelectron spectroscopy (UPS) is a very similar technique to XPS that makes use of much lower energy photons to emphasis variations in the low energy valence band electronic structure. [Pg.591]


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See also in sourсe #XX -- [ Pg.205 ]

See also in sourсe #XX -- [ Pg.524 , Pg.525 ]

See also in sourсe #XX -- [ Pg.304 ]




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