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Intermediate coupling states

An accurate procedure for performing calculations that incorporate spin-orbit and other relativistic effects, and that represents intermediate coupling states for molecules containing heavy atoms, is based on A-S coupling in conjunction with the use of the ab initio REP-based spin-orbit operator and extended configuration interaction. The coupling scheme is more familiar than co-co coupling to chemists and physicists. In addition, the complexity of calculations necessary to achieve reliable results is computationally tractable. [Pg.178]

Table I. g-values and Ueff of ground states In Russell-Saunders and intermediate coupling for different configurations. Table I. g-values and Ueff of ground states In Russell-Saunders and intermediate coupling for different configurations.
Due to the intermediate coupling the sign of the crystal field matrix element 6 is reversed compared to the pure Russell-Saunders state. Thus for 8-fold cubic coordination a F7 ground state was found. From EPR measurements on Pu3"1" diluted in fluorite host lattices, a magnetic moment at T=0 K can be calculated, ranging from li ff = 1.333 (in Ce02) to y ff = 0.942 (in SrCl2) (24,... [Pg.41]

An intermediate spin state (a quartet 4A2) similarly is feasible for five-coordinate iron(III) though, as pointed out by Kahn [118], the situation may be more complex. If the states are close in energy then they can interact through spin-orbit coupling to give a so-called spin-admixed ground state. [Pg.38]

The X coupling parameter defines a set of intermediate hybrid states between the unperturbed and the fully perturbed states. Then, the total change in the free energy is... [Pg.143]

Hamiltonian quantum states. Two situations can be envisaged. In the first one, the system moves stepwise from the APC states to the interconversion complex. We assume that the i-th state of the active precursor is populated i f > at a given time to, and if f> is intermediate Hamiltonian state that are coupled by the electro-magnetic field. [Pg.327]

A suitable comparison of the Os(VI)/ Os(III) couple is the well-studied three-electron oxidant HCr04, where the intermediate oxidation states Cr(V)/Cr(IV) appear to be unstable with respect to disproportionation. However, the Os system shows a dramatically enhanced electrochemical reversibihty compared to Cr(IV). This feature may play an important role in the ability of related systems that act as redox catalysts. [Pg.569]

We take as an example the case of plutonium monopnictides PuP, PuAs, PuSb, the susceptibility of which is well fitted by Eq, (17). Results are given in Table 8 while bare data are in agreement with the full J multiplet value ( 1 pP in the intermediate coupling), the corrected value is substantially smaller and points towards a Fg ground state (see Table 8) in agreement with more detailed discussions ... [Pg.144]

Due to the localization of the 5 f electrons in the oxides a final state multiplet structure is expected. Therefore, these spectra have been compared with final state intensities calculated in an intermediate coupling scheme which accoimts for the strong spin-orbit... [Pg.245]

Even AS = 2 transitions in excited states can be rapid. In ground state spin equilibria these transitions can be nonadiabatic due to the requirement of mixing through spin-orbit coupling with excited intermediate spin states. In photophysical processes these excited states can actually be populated. Again this conclusion follows from the success of photoperturbation methods applied to AS = 2 spin equilibria. For example, excitation of the singlet state of iron(II) results in detectable population of the quintet spin-equilibrium state more rapidly than... [Pg.47]

The solution is summarized in Figure 8.1. The4F state has L 3, and so (from Tabic 7.1) it is split by an intermediate field into three states which belong to the IRs A2 Ti T2 =r2 r4 r5. To examine the effect of spin—orbit coupling on these intermediate-field states, we use the fact that if -tp fi"fi, where fi forms a basis for T and x1 forms a basis for F, then ip = fix forms a basis for the direct product (DP) representation F F. Here S=3/2, and the representation 1 / is Tg (Table 8.2). Take the DPs of Tg with 1 2, T4, and P to obtain... [Pg.152]


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See also in sourсe #XX -- [ Pg.2 , Pg.173 ]




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Coupling states

Intermediate state

Predissociation for a pair of states intermediate between adiabatic and diabatic coupling limits

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