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Group theory representation reduction

Thus, any representation Tcan be expressed as a function of its irreducible representations Pi. This operation is written as P = S a, Pi, where a, indicates the number of times that Pi appears in the reduction. In group theory, it is said that the reducible representation P is reduced into its Pi irreducible representations. The reduction operation is the key point for applying group theory in spectroscopy. To perform a reduction, we need to use the so-called character tables. [Pg.241]

To tackle this problem, we first need to know how a given representation F is reduced to its irreducible representations T) in other words, to determine the coefficients a, in the equation F= Sat Fi. Although this is a key problem in group theory, here we only explain how to perform this reduction without entering into formal details, which can easily be found in specialized textbooks. [Pg.244]

The previous example has shown how group theory can be used in a symmetry reduction problem. This symmetry reduction also occurs when an ion is incorporated in a crystal. We will now treat how to predict the number of energy levels of the ion in the crystal (the active center) and how to properly label these levels by irreducible representations. [Pg.249]

N. Chriss and V. Ginzburg, Representation theory and complex geometry (Geometric techniques in representation theory of reductive groups) , Progress in Math. Birkhauser, (to appear). [Pg.113]

In applying the methods of group theory to problems related to molecular structure or dynamics, the procedure that is followed usually involves deriving a reducible representation for the phenomenon of interest, such as molecular vibration, and then decomposing it into its irreducible components. (A reducible representation will always be a sum of irreducible ones.) Although the decomposition can sometimes be accomplished by inspection, for the more general case, the following reduction... [Pg.43]

It is important to note that no symmetry operation exchanges an axial ligands with an equatorial one. As these two types of ligands are therefore non-equivalent, both chemically and according to group theory, they can he considered separately. The characters of the representations Per (eq) and P (ax) are given in Table 6.22. From the reduction formula (6.5), we find ... [Pg.239]


See other pages where Group theory representation reduction is mentioned: [Pg.247]    [Pg.470]    [Pg.17]    [Pg.249]    [Pg.62]    [Pg.30]    [Pg.20]    [Pg.133]    [Pg.153]    [Pg.499]    [Pg.132]    [Pg.267]    [Pg.423]    [Pg.526]    [Pg.165]    [Pg.110]    [Pg.8088]    [Pg.1138]   
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