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Ta point group

The remaining eight vectors, xi,. .., X4 andyi,. .., y>4, will form eight linear combinations having symmetries E, T, and T2. In order to see how these ligand vectors transform under the 24 symmetry operations of the Ta point group, the direction numbers of all the ligand vectors are required. They are... [Pg.229]

Table B.4. Double group characters table for the Ta point group. The numbers before the symmetry operations correspond to the number of geometrically different axes or symmetry planes. Some of the operations of the double group belong to the same class as those of the original group. When more than one IR is indicated, the first one corresponds to the notation of Mulliken [11], the second one to Koster et al. [9] and the one in parentheses to [3]... Table B.4. Double group characters table for the Ta point group. The numbers before the symmetry operations correspond to the number of geometrically different axes or symmetry planes. Some of the operations of the double group belong to the same class as those of the original group. When more than one IR is indicated, the first one corresponds to the notation of Mulliken [11], the second one to Koster et al. [9] and the one in parentheses to [3]...
Problem 6.5 The Other greenhouse gas mentioned above is CH4, which belongs to the Ta point group. Using the basis shown in Figure 6.8, demonstrate that the C—H stretching modes of this molecule have the reducible representation shown ... [Pg.176]

Pig. 4. Group of twelve aluminum octahedra, point-group symmetry Ta, occurring in zunyite. [Pg.548]

A planar molecule of point group 03b is shown in Fig. 5. The sigma orbitals i, <72 and (73 represented there will be taken as the basis set Application of the method developed in Section 8.9 yields the characters of the reducible representation given in Table 14. With the use of the magic formula (Eq. (37)] the structure of the reduced representation is of the form Ta — A, ... [Pg.319]

Vibrations may be decomposed into three orthogonal components Ta (a = x, y, z) in three directions. These displacements have the same symmetry properties as cartesian coordinates. Likewise, any rotation may be decomposed into components Ra. The i.r. spanned by translations and rotations must clearly follow the appropriate symmetry type of the point-group character table. In quantum formalism, a transition will be allowed only if the symmetry product of the initial and final-state wave functions contains the symmetry species of the operator appropriate to the transition process. Definition of the symmetry product will be explained in terms of a simple example. [Pg.298]

Ta,Tp.Te of the molecular point group vanishes if the direct-product... [Pg.232]

Although most molecules in point groups /ft, 0, Ta, C, C and C may be assigned by inspection, some appear unusual. Consider the cubic symmetry of cubane. CBH8. To... [Pg.591]

RetinalS. The structure and photophysics of rhodopsins are intimately related to the spectroscopic properties of their retiny1-polyene chromophore in its protein-free forms, such as the aldehyde (retinal), the alcohol (retinol or vitamin A), and the corresponding Schiff bases. Since most of the available spectroscopic information refers to retinal isomers (48-55), we shall first center the discussion on the aldehyde derivatives. Three bands, a main one (I) around 380 nm and two weaker transitions at 280 nm and 250 nm (II and III), dominate the spectrum of retinals in the visible and near ultraviolet (Fig. 2). Assignments of these transitions are commonly made in terms of the lowest tt, tt excited states of linear polyenes, the spectroscopic theories of which have been extensively discussed in the past decade (56-60). In terms of the idealized C2h point group of, for example, all-trans butadiene, transitions are expected from the Ta ground state to B , A, and A" excited states... [Pg.105]

In accordance with what was shown in Eq. 7.3.5 these three expressions are the three components of an axial vector that is, the above expressions will transform like Rx, Ry, and Rz, respectively, in any point group that has the symmetry of F. This can be verified in a straightforward manner by showing that, say (Rx, is invariant under an improper rotation by an angle 6 about the x axis. Since F is invariant under this transformation Ta, we may write... [Pg.142]

In addition to the 10 point groups mentioned above there are 10 more point groups that lack a center of inversion but are not polar. These are Csh, d2,3,4,6,2d 3h/ S4, t and ta- or 6, 222, 32,422,622,42m, 62m, 4,23, and 43m. Crystals in this class, when distorted, may produce a dipole and are called piezoelectrics. Therefore, all ferroelectrics and pyroelectrics are also piezoelectrics, but not all piezoelectrics are pyroelectrics or ferroelectrics. [Pg.452]

Na and Nb are the numbers of atoms in the two groups A and B and S is the switching function. With the group-based switching function, it is necessary to define the distance between the two groups (i.e. the two points Ta and Tb). There is no definitive way to do this. As with cutoffs, a special marker atom can be nominated within each residue, or the centre of mass, centre of geometry or centre of charge may be used. [Pg.347]

A decrease in metal-carbon distances when going down a group has also been pointed out. However, if this observation can roughly be applied to Zr and Hf (owing to lanthanide contraction), it does not fit the data obtained for Ti (Table 11.1). In contrast, for tetracoordinated complexes of the third transition row, replacement of just one neopentyl ligand is reported only when silica was pretreated at 700°C [18, 19, 23, 24]. For the tantalum complex [Ta(=CHCMe3)Np3, its... [Pg.421]


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See also in sourсe #XX -- [ Pg.67 , Pg.78 ]




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