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Magnetic valence model

The second group comprises calculations of the band structures and related properties. This also includes the so-called magnetic valence model , which is a modification of the band approach. [Pg.252]

Until about 20 years ago, the valence bond model discussed in Chapter 7 was widely used to explain electronic structure and bonding in complex ions. It assumed that lone pairs of electrons were contributed by ligands to form covalent bonds with metal atoms. This model had two major deficiencies. It could not easily explain the magnetic properties of complex ions. [Pg.416]

This example shows that dipolar interactions can produce unexpected effects in systems containing polynuclear clusters, so that their complete quantitative description requires a model in which the dipolar interactions between all the paramagnetic sites of the system are explicitly taken into account. Local spin models of this kind can provide a description of the relative arrangement of the interacting centers at atomic resolution and have been worked out for systems containing [2Fe-2S] and [4Fe-4S] clusters (112, 192). In the latter case, an additional complication arises due to the delocalized character of the [Fe(III), Fe(II)] mixed-valence pair, so that the magnetic moments carried by the two sites A and B of Fig. 8B must be written... [Pg.464]

We have not mentioned open shells of electrons in our general considerations but then we have not specifically mentioned closed shells either. Certainly our examples are all closed shell but this choice simply reflects our main area of interest valence theory. The derivations and considerations of constraints in the opening sections are independent of the numbers of electrons involved in the system and, in particular, are independent of the magnetic properties of the molecules concerned simply because the spin variable does not occur in our approximate Hamiltonian. Nevertheless, it is traditional to treat open and closed shells of electrons by separate techniques and it is of some interest to investigate the consequences of this dichotomy. The independent-electron model (UHF - no symmetry constraints) is the simplest one to investigate we give below an abbreviated discussion. [Pg.80]


See other pages where Magnetic valence model is mentioned: [Pg.144]    [Pg.259]    [Pg.376]    [Pg.376]    [Pg.144]    [Pg.259]    [Pg.376]    [Pg.376]    [Pg.186]    [Pg.2459]    [Pg.120]    [Pg.2458]    [Pg.261]    [Pg.153]    [Pg.69]    [Pg.65]    [Pg.187]    [Pg.216]    [Pg.4]    [Pg.428]    [Pg.445]    [Pg.467]    [Pg.468]    [Pg.469]    [Pg.479]    [Pg.2]    [Pg.426]    [Pg.225]    [Pg.134]    [Pg.147]    [Pg.3]    [Pg.193]    [Pg.53]    [Pg.148]    [Pg.344]    [Pg.218]    [Pg.459]    [Pg.509]    [Pg.195]    [Pg.376]    [Pg.452]    [Pg.228]    [Pg.31]    [Pg.207]    [Pg.301]    [Pg.12]    [Pg.48]    [Pg.272]    [Pg.296]   
See also in sourсe #XX -- [ Pg.375 , Pg.376 ]




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