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Valence Mechanisms

First we focus on the mechanisms that arise from interactions among the configurations in the active space, restricting ourselves to the role played by the two Cu + ions. For this centro-symmetric system, the active orbitals g = (a + b)l and u = a — b) pi shown in Fig. 5.1 define four different determinants [Pg.142]

The diagonalization of the corresponding 4x4 matrix produces four eigenstates, three singlets and one triplet [Pg.142]

1 Demonstrate by substitution that Sg is dominated by the neutral determinants when X ji.. What situation is described for A. 2 /i  [Pg.142]

The energy difference of Sg and Tu defines / but the analysis is much easier in a representation with localized orbitals. Therefore, we rewrite the CAS in terms of the orthogonal localized Cu orbitals a and b, shown in Fig. 5.2. By defining the following electronic structure parameters [Pg.142]

Here Eref = haa + hbb + Jab is the reference energy and has been subtracted from all diagonal matrix elements. Kab is the direct exchange, U is the on-site repulsion parameter and tab is the hopping integral and gives a measure of the probability for the electron hopping from site aiob and vice-versa. [Pg.143]


The introduction of Me2X into FbX generates a proportional number of anion vacancies which are an obstacle to an increase in the valence of lead and, once again, p-t3q>e conduction is not obtained. The controlled valence mechanism, which increases the charge of the lead ions, is effective only if the excess sulfur, selenium, or tellurium is not less than that required to form Me2X with the same cation-anion ratio as the host substance ... [Pg.146]

This sum of terms can be represented by means of corresponding diagrams (see fig. 3). The first term in (4.35) (fig. 3a) describes the mixing of the compound nucleus states caused by the TNPC interaction [76-78]. The second term describes the T-violating decay (fig. 3b) of a compound resonance into the channel jS. The third term (fig. 3c) corresponds to the direct (potential scattering) process caused by the TNPC interaction. The expression is more complicated for the valence mechanism of T violation, which is described by fig. 3e. [Pg.99]

An increased-valence mechanism for the reaction does not have these... [Pg.285]

Figure 22-1 Increased-valence mechanism for oxidation of Fe(II) porphyrin complexes by O2 to form p-oxo bridged dimers. Figure 22-1 Increased-valence mechanism for oxidation of Fe(II) porphyrin complexes by O2 to form p-oxo bridged dimers.
The electron-spin theory which is appropriate for the increased-valence mechanism of 1,3 dipolar cycloaddition is (iescribed in some detail in Ref 11, where the importance of the long-bond structures (such as (26)) for the electronic stracture and reactivity of any 1,3 dipolar molecule has also been stressed. The latter conclusion has received support from a number of valence-bond calculations and Goddard and Walch have used structure (26) alone to represent the electronic structure of CHjNj. [Pg.293]

Dislocation theory as a portion of the subject of solid-state physics is somewhat beyond the scope of this book, but it is desirable to examine the subject briefly in terms of its implications in surface chemistry. Perhaps the most elementary type of defect is that of an extra or interstitial atom—Frenkel defect [110]—or a missing atom or vacancy—Schottky defect [111]. Such point defects play an important role in the treatment of diffusion and electrical conductivities in solids and the solubility of a salt in the host lattice of another or different valence type [112]. Point defects have a thermodynamic basis for their existence in terms of the energy and entropy of their formation, the situation is similar to the formation of isolated holes and erratic atoms on a surface. Dislocations, on the other hand, may be viewed as an organized concentration of point defects they are lattice defects and play an important role in the mechanism of the plastic deformation of solids. Lattice defects or dislocations are not thermodynamic in the sense of the point defects their formation is intimately connected with the mechanism of nucleation and crystal growth (see Section IX-4), and they constitute an important source of surface imperfection. [Pg.275]

For this reason, there has been much work on empirical potentials suitable for use on a wide range of systems. These take a sensible functional form with parameters fitted to reproduce available data. Many different potentials, known as molecular mechanics (MM) potentials, have been developed for ground-state organic and biochemical systems [58-60], They have the advantages of simplicity, and are transferable between systems, but do suffer firom inaccuracies and rigidity—no reactions are possible. Schemes have been developed to correct for these deficiencies. The empirical valence bond (EVB) method of Warshel [61,62], and the molecular mechanics-valence bond (MMVB) of Bemardi et al. [63,64] try to extend MM to include excited-state effects and reactions. The MMVB Hamiltonian is parameterized against CASSCF calculations, and is thus particularly suited to photochemistry. [Pg.254]

The concept of biradicals and biradicaloids was often used in attempts to account for the mechanism of photochemical reactions [2,20,129-131]. A biradical (or diradical) may be defined as [132] an even-electron molecule that has one bond less than the number permitted by the standard rules of valence. [Pg.388]

Th e ability to perform m oleciilar orbital (MO ) calculation s on m et-als is extremely useliil because molecular mechanics methods are gen erally unable to treat m etals. This is becau se m etals h ave a wide range of valences, oxidation states, spin multiplicities, and have 1111 usual bonding situations (e.g.. d%-p% back bonding). In addition. the 11 on direction al n at are o ( m etallic hon din g is less am en a-ble to a ball and spring interpretation. [Pg.151]

Much of quantum chemistry attempts to make more quantitative these aspects of chemists view of the periodic table and of atomic valence and structure. By starting from first principles and treating atomic and molecular states as solutions of a so-called Schrodinger equation, quantum chemistry seeks to determine what underlies the empirical quantum numbers, orbitals, the aufbau principle and the concept of valence used by spectroscopists and chemists, in some cases, even prior to the advent of quantum mechanics. [Pg.7]

The consistent force field (CFF) was developed to yield consistent accuracy of results for conformations, vibrational spectra, strain energy, and vibrational enthalpy of proteins. There are several variations on this, such as the Ure-Bradley version (UBCFF), a valence version (CVFF), and Lynghy CFF. The quantum mechanically parameterized force field (QMFF) was parameterized from ah initio results. CFF93 is a rescaling of QMFF to reproduce experimental results. These force fields use five to six valence terms, one of which is an electrostatic term, and four to six cross terms. [Pg.54]

Semi-empirical quantum mechanics methods have evolved over the last three decades. Using today s microcomputers, they can produce meaningful, often quantitative, results for large molecular systems. The roots of the methods lie in the theory of % electrons, now largely superseded by all-valence electron theories. [Pg.31]

HyperChem quantum mechanics calculations must start with the number of electrons (N) and how many of them have alpha spins (the remaining electrons have beta spins). HyperChem obtains this information from the charge and spin multiplicity that you specify in the Semi-empirical Options dialog box or Ab Initio Options dialog box. N is then computed by counting the electrons (valence electrons in semi-empirical methods and all electrons in fll) mitio method) associated with each (assumed neutral) atom and... [Pg.44]

In absorption spectroscopy a beam of electromagnetic radiation passes through a sample. Much of the radiation is transmitted without a loss in intensity. At selected frequencies, however, the radiation s intensity is attenuated. This process of attenuation is called absorption. Two general requirements must be met if an analyte is to absorb electromagnetic radiation. The first requirement is that there must be a mechanism by which the radiation s electric field or magnetic field interacts with the analyte. For ultraviolet and visible radiation, this interaction involves the electronic energy of valence electrons. A chemical bond s vibrational energy is altered by the absorbance of infrared radiation. A more detailed treatment of this interaction, and its importance in deter-... [Pg.380]


See other pages where Valence Mechanisms is mentioned: [Pg.525]    [Pg.142]    [Pg.203]    [Pg.145]    [Pg.187]    [Pg.525]    [Pg.142]    [Pg.203]    [Pg.145]    [Pg.187]    [Pg.312]    [Pg.1324]    [Pg.2222]    [Pg.2342]    [Pg.308]    [Pg.46]    [Pg.185]    [Pg.244]    [Pg.266]    [Pg.631]    [Pg.632]    [Pg.156]    [Pg.32]    [Pg.8]    [Pg.285]    [Pg.364]    [Pg.137]    [Pg.139]    [Pg.34]    [Pg.167]    [Pg.194]    [Pg.160]    [Pg.295]    [Pg.412]   


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