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Dimension of a representation

The dimension of a representation is the same as the order of the matrix. To reduce a representation it is necessary to reduce its order. It is noted that the dimension of a matrix representation corresponds to the character of the identity (E) matrix. [Pg.296]

A standard tableau is defined as one in which the numbers increase when one reads from left to right in each row and from top to bottom in each column. It can be shown Mi) that the dimension of a representation is equal to the number of standard tableaux associated with the corresponding diagram. The reader is also referred to the literature Mi) for methods of calculating characters of the representations from the diagrams. [Pg.31]

In the so-calledMu/Z/ten notation, representations A and B (which does not appear in Table 7.2) are mono-dimensional, E representations are bi-dimensional, and T representations are three-dimensional. Other irreducible representations of higher order are G (three-dimensional) and H (tetra-dimensional). We will also state now that the dimension of a representation gives the degeneracy of its associated energy level. [Pg.244]

Letters These tell you about the number of dimensions (also called the degeneracy) of the representation (row of numbers). The dimension of a representation is simply the value under E on the character table. Because all molecules have an identity operation ( ), E is always listed as the first class of symmetry elements (the first column of numbers). For the dimensions of all four representations are 1 (or, every row has a value of 1 under E), so you would expect the letter of the Mulliken symbol for each representation to be either an A or a B ... [Pg.111]

Case (b) aproduces a set of functions t/rj, which is independent of the set but which also forms a basis for A (u) of H. The irreducible co-representation D of G corresponds again to a single irreducible representation of H, but has twice its dimension. In this case the dimension of A (u) is doubled. [Pg.733]

Fig. 75.—Vectorial representation in two dimensions of a freely jointed chain. A random walk of fifty steps. Fig. 75.—Vectorial representation in two dimensions of a freely jointed chain. A random walk of fifty steps.
As shown earlier, the operation is always in a class by itself, as it commutes with all other operations of the group. It is identified with Ti, the arbitrarily chosen first class of operation In a given representati.Qnt ie operation E corresponds to a. unit matrix whose order is equal to the dimension of the representation. Hence, the esultipg character, the sums of e diagonal elements, is also equal to the dimension of the representation, The dimension of each representation can thus be easily determined by inspection of the corresponding entry in the first column of characters in the table. [Pg.105]

Since Lm is invariant under G, any operator A G transforms each vector >n Lm into another vector in Lm. Hence, the operation AM results in a matrix of the same form as T(A). It should be clear that the two sets of matrices I) 1) and D > give two new representations of dimensions m and n — m respectively for the group G. For there exists a set of basis vectors l, n] for rX2 The representation T is said to be reducible. It follows that the reducibility of a representation is linked to the existence of a proper invariant subspace in the full space. Only the subspace of the first m components is... [Pg.73]

Not only are linear transformations necessary for the very definition of a representation in Chapter 6, but they are useful in calculating dimensions of vector spaces — see Proposition 2.5. Linear transformations are at the heart of homomorphisms of representations and many other constructions. We will often appeal to the propositions in this section as we construct linear transformations. For example, we will use Proposition 2.4 in Section 5.3 to define the tensor product of representations. [Pg.51]

The matrices of (9.25) are not the only matrices that multiply in the same manner as the S3v group operations, as we shall shortly see. Any set of nonnull square matrices that multiply in the same way as the elements of a given group is said to form a representation of that group. The order of the matrices is called the dimension of the representation. To form a representation, the correspondence between matrices and group elements need not be one-to-one rather, a given matrix can correspond to more... [Pg.454]

Let us now consider the irreducible representations of several typical groups to see how these rules apply. The group C2v consists of four elements, and each is in a separate class. Hence (rule 5) there are four irreducible representations for this group. But it is also required (rule 1) that the sum of the squares of the dimensions of these representations equal h. Thus we are looking for a set of four positive integers, /b /2, /3, and /4, which satisfy the relation... [Pg.84]

Figure 17.3. Energy bands for the simple cubic Bravais lattice in the free-electron approximation at A on rx. The symmetry of the eigenfunctions at T and at X given in the diagram satisfy compatibility requirements (Koster et al. (1963)). Degeneracies are not marked, but may be easily calculated from the dimensions of the representations. Figure 17.3. Energy bands for the simple cubic Bravais lattice in the free-electron approximation at A on rx. The symmetry of the eigenfunctions at T and at X given in the diagram satisfy compatibility requirements (Koster et al. (1963)). Degeneracies are not marked, but may be easily calculated from the dimensions of the representations.
The commonly employed methods are known in the literature as periodic boundary condition (PBC) and minimum imaging. " Essentially, the way to remove surfaces is to allow the atoms near opposite surfaces to interact as if they were near neighbors, that is, to create a flat torus in d + 1 dimensions, where d is the dimension of a space. A pictorial representation of minimum imaging can be found in Figure 12. In this section, we discuss the application of these boundary conditions for a simulation cell of arbitrary shape. [Pg.355]

Fig. 1 (a) y-CD chemical structure and approximate dimensions of a-, P-, and y- CDs schematic representation of packing structures of (c) cage-type, (d) layer-type, and (e) head-to-tail channel-type CD crystals and (f) CD-IC channels containing included polymer guests... [Pg.117]

The number of chemical reactants determines the dimension of a chemical system. The minimum number is necessarily one, however the interaction between the elements is interesting thus systems with at least two reactants is relevant in the context of the present paper. In mathematical terms, a solution is a line represented by x = x t) as a function of time element. Representation of this solution has been in basically two different forms which will be discussed below ... [Pg.57]

The C2v consist of 4 element and each is in a separate class. Hence according to rule there will be four irreducible representations for the group and according to rule the sum of the squares of dimensions of these representations equals to g. Thus... [Pg.10]


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See also in sourсe #XX -- [ Pg.98 ]




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