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Groups representations

Note that every matrix in the four dimensional group representation labeled DN) has the so-called block diagonal form... [Pg.586]

This means that these matriees are really a eombination of two separate group representations (mathematieally, it is ealled a direet sum representation). We say that Dl ) is redueible into a one-dimensional representation DlO and a three-dimensional representation formed by the 3x3 submatriees whieh we will eall Dl ). [Pg.587]

We could take any set of functions as a basis for a group representation. Commonly used sets include coordinates (x,y,z) located on the atoms of a polyatomic molecule (their symmetry treatment is equivalent to that involved in treating a set of p... [Pg.590]

Case (a). This case includes all real single-group representations, with real character and dimension greater than 1. [Pg.737]

Case (b). This case includes no single-group representations, and all real one-dimensional, double-group representations. This includes only the following. [Pg.737]

Case (c). This case includes all single- and double-group representations with complex character. [Pg.737]

Dominant-diagonal theorem, 58 Doob, J. L., 171,174,269 Dorodnitzin, A., 388 Double-group representations, 737 Double groups, 727... [Pg.773]

Single-group representations, 737 Singleton, Richard (7., 282 Singular points, 324 elementary, 324 principal, 327 simple, 328... [Pg.783]

L. Domhoff, Group Representation Theory. Part A Ordinary Representation Theory. Part B Modular Representation Theory (1971,1972)... [Pg.767]

Since S is a symmetric matrix equal to Q(0), these equalities show that the off-diagonal blocks must vanish at x = 0, and hence that there is no instantaneous coupling between variables of opposite parity. The symmetry or asymmetry of the block matrices in the grouped representation is a convenient way of visualizing the parity results that follow. [Pg.12]

These show that in the grouped representation, the even temporal part of the matrices is block-diagonal, and the odd temporal part is block-adiagonal, (i.e., the diagonal blocks are zero). Also, as matrices of second derivatives with respect to the same variable, A(x) and A (x) are symmetric. The even temporal part of B is symmetric, and the odd part is antisymmetric. [Pg.13]

Here and throughout, x = sign(x). These are small-time expansions, but they are not Taylor expansions, as the appearance of nonanalytic terms indicates. From the parity and symmetry rules, the odd coefficients are block-adiagonal, and the even coefficients are block-diagonal in the grouped representation. Equating the coefficients of x / x in Eqs. (28) and (29), it follows that... [Pg.15]

This follows because, in the grouped representation, Q+ contains nonzero blocks only on the diagonal and is symmetric, and Q contairisnonzero blocks only off the diagonal and is asymmetric. These symmetry rules are called the Onsager-Casimir reciprocal relations [10, 24], They show that the magnitude of the coupling coefficient between a flux and a force is equal to that between the force and the flux. [Pg.19]

Thus the sum of the diagonal elements, or trace, of a matrix D(R) is invariant under a transformation of the coordinate axes. When dealing with group representations the trace Dtl(R) is called the character of R in the... [Pg.72]

This equation (16) is known as the great orthogonality theorem for the irreducible representations of a group and occupies a central position in the theory of group representations. [Pg.79]

H.F. Jones, Groups, Representations and Physics, 1990,M Hilger, Bristol. M... [Pg.523]

Barut, A. O., and Raczka, R. (1986), Theory of Group Representations and Applications, World Scientific, Singapore. [Pg.222]

Vilenkin, N. I. (1968), Special Functions and the Theory of Group Representations, Transl. Math. Monogr., Am. Math. Soc. 22, Providence. [Pg.235]

In particular, a group of numbers isomorphic to a symmetry group is an example of a representation of the symmetry group. Group representations are of the utmost importance in chemistry because they make it possible to achieve the effects of geometrical reasoning by means of calculations with the numerical representations. [Pg.9]

The theory of group representation proves a number of results. [Pg.68]


See other pages where Groups representations is mentioned: [Pg.583]    [Pg.121]    [Pg.744]    [Pg.751]    [Pg.332]    [Pg.218]    [Pg.102]    [Pg.226]    [Pg.149]    [Pg.39]    [Pg.41]    [Pg.41]    [Pg.41]    [Pg.43]    [Pg.45]    [Pg.47]    [Pg.49]    [Pg.52]    [Pg.128]    [Pg.128]    [Pg.63]    [Pg.670]    [Pg.525]    [Pg.64]    [Pg.111]   
See also in sourсe #XX -- [ Pg.71 ]

See also in sourсe #XX -- [ Pg.39 , Pg.41 ]

See also in sourсe #XX -- [ Pg.62 ]




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Co-representations of magnetic point groups

Cubic group representation

Double group representation

Faithful representation group

Group algebraic representation of the antisymmetrizer

Group theory irreducible representations

Group theory representation reduction

Group, Abelian representation

Group, characters representation

Groups irreducible matrix representations

Groups irreducible representation

Groups matrix representations

Groups reducible representation

Groups, Abelian, irreducible representations

Groups, continuous irreducible representations

Heisenberg group representation

Induced Representations of Space Groups in q-basis

Irreducible Representations of Translation Group Brillouin Zone

Irreducible representation of a group

Irreducible representations group theoretical properties

Isomorphic representation group

Lie group representation

Matrix representation of groups

Properties and Representations of Groups

Reducible representation of a group

Reducible representations group orbitals from

Representation of a group

Representation of the group

Representation point-group

Representations for Cyclic Groups

Representations for Cyclic and Related Groups

Representations of Finite Groups

Representations of Space Groups

Representations of point groups

Representations of the rotation group

Representations, of groups

Rotation group irreducible representations

Site Symmetry and Induced Representations of Space Groups

Space group representations

Space group symmetry and its mathematical representation

Spinor representations of space groups

Totally symmetric representation of a group

Unfaithful representation group

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