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Block-form matrices

What is not so obvious is that since the block structure is identical for every symmetry operation, the individual blocks themselves, written as matrices, form lower dimensional representations. Take, for example, the block form matrices... [Pg.96]

Another feature of block form matrices is that if a matrix A is in the block form [AJ [0] [Q]... [Pg.97]

We will return to the topic of block form matrices in the next chapter it is the foundation of most of the theorems which follow. [Pg.97]

In matrix block form the equations that govern the time evolution of the parameters can be expressed as... [Pg.225]

The Material of the Example. Poly(ether ester) (PEE) materials are thermoplastic elastomers. Fibers made from this class of multiblock copolymers are commercially available as Sympatex . Axle sleeves for automotive applications or gaskets are traded as Arnitel or Hytrel . Polyether blocks form the soft phase (matrix). The polyester forms the hard domains which provide physical cross-linking of the chains. This nanostructure is the reason for the rubbery nature of the material. [Pg.172]

Fig. 9 Schematic representation of three approaches to generate nanoporous and meso-porous materials with block copolymers, a Block copolymer micelle templating for mesoporous inorganic materials. Block copolymer micelles form a hexagonal array. Silicate species then occupy the spaces between the cylinders. The final removal of micelle template leaves hollow cylinders, b Block copolymer matrix for nanoporous materials. Block copolymers form hexagonal cylinder phase in bulk or thin film state. Subsequent crosslinking fixes the matrix hollow channels are generated by removing the minor phase, c Rod-coil block copolymer for microporous materials. Solution-cast micellar films consisted of multilayers of hexagonally ordered arrays of spherical holes. (Adapted from [33])... Fig. 9 Schematic representation of three approaches to generate nanoporous and meso-porous materials with block copolymers, a Block copolymer micelle templating for mesoporous inorganic materials. Block copolymer micelles form a hexagonal array. Silicate species then occupy the spaces between the cylinders. The final removal of micelle template leaves hollow cylinders, b Block copolymer matrix for nanoporous materials. Block copolymers form hexagonal cylinder phase in bulk or thin film state. Subsequent crosslinking fixes the matrix hollow channels are generated by removing the minor phase, c Rod-coil block copolymer for microporous materials. Solution-cast micellar films consisted of multilayers of hexagonally ordered arrays of spherical holes. (Adapted from [33])...
In this basis, the rotation-vibration matrix has a block form. For example, the matrix (4.131) becomes... [Pg.116]

Ehcpress the orbitals as [Pg.25]

In the case of the representation of C3 in Figure 6.2, it is obvious that the matrices are merely combinations of of simpler representations. But if the three matrices were subjected to a similarity transformation, they would no longer be in block form, and it would not be obvious that the representation is composite. Applying the reverse similarity transformation would put the matrices back into block form. If there exists a similarity transformation such that applying it to each matrix in a representation puts every matrix into congruent block form, the representation is said to be reducible. If no such similarity transformation exists, the representation is said to be irreducible. [Pg.44]

This representation is in block form, and is obviously reducible. Consider another coordinate system, rotated in the a — y plane by 45°. Verify that in this new coordinate system the formulas giving the effect of cr are a —y and y —s- —x. Find the matrix relating the two coordinate systems and verify that a similarity transformation applied to the matrices of this new representation produces the old representation. How does this demonstrate the reducibility of the new representation ... [Pg.45]

Pauli principle will ensure that no extra terms occur due to such a mixing. The transformation matrix for orbital set A then has the following blocked form ... [Pg.243]

First we observe that any matrix is similar to a block diagonal matrix, where the sub-matrices along the main diagonal are Jordan blocks. It is thus sufficient to prove that any Jordan block can be transformed to a complex symmetric matrix. In passing we note that any matrix with distinct eigenvalues can be brought to diagonal form by a similarity transformation. The key study therefore relates to XI + J (0), where 1 is the n-dimensional unit matrix and... [Pg.99]

X-ray diffraction cannot distinguish the different blocks and is not able to say which types of blocks form the cylinders and the matrix. On the contrary,... [Pg.93]

A submatrix is formed at each point on the grid, relating the concentration of each species to the others (kinetically). The material balance equation for all the species may be written with this submatrix down the diagonal - resulting in a block tridiagonal matrix. This may be solved using a matrix version of the Thomas algorithm which requires each submatrix to be inverted (by LU factorization). [Pg.91]

Topological matrix of a bipartite graph. Bipartite graphs, just as the corresponding alternant systems, possess a number of remarkable properties. In particular, their vertices can always be enumerated so that the topological matrix is simplified and reduced to the block form... [Pg.50]

The maUix composed of the eigenvalues of topological matrix of a bipartite graph whose vertices are properly enumerated also takes the sufficiently simple block form ... [Pg.53]

The topological matrix of this alternant system is then written in a block form as follows ... [Pg.60]

If a transformation matrix S can be found which transforms the matrices D(i) of a given representation to a block-factored matrix form, this representation is considered to be reducible. [Pg.47]

Finally, we comment briefly on the use of symmetry. By making use of the symmetry point group of the molecule, the Fock matrix may be transformed into a blocked form and the eigenvalue problem (3.1) is then solved block by block. Transformation into a blocked form may be performed in different ways which will be not discussed here. We note only that the gain is not very important since the time involved in... [Pg.70]


See other pages where Block-form matrices is mentioned: [Pg.271]    [Pg.2929]    [Pg.2929]    [Pg.219]    [Pg.330]    [Pg.178]    [Pg.150]    [Pg.150]    [Pg.226]    [Pg.147]    [Pg.97]    [Pg.46]    [Pg.112]    [Pg.177]    [Pg.121]    [Pg.212]    [Pg.163]    [Pg.269]    [Pg.293]    [Pg.215]    [Pg.610]    [Pg.340]    [Pg.95]    [Pg.97]    [Pg.168]    [Pg.169]    [Pg.90]    [Pg.654]    [Pg.166]    [Pg.178]    [Pg.95]    [Pg.97]    [Pg.282]   
See also in sourсe #XX -- [ Pg.4 , Pg.2929 ]




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