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Rotational inversion symmetry

Symmetry elements include axes of twofold, threefold, fourfold, and sixfold rotational symmetry and mirror planes. There are also axes of rotational inversion symmetry. With these, there are rotations that cause mirror images. For example, a simple cube has three <100> axes of fourfold symmetry, four axes of <111>... [Pg.12]

Figure 3.7 demonstrates this rotation inversion symmetry operation in space lattices. [Pg.22]

Define the following terms symmetry operation, symmetry element, principal axis, identity operation, improper rotation, inversion, symmetry group, point group, conjugate elements, similarity transformation and class. [Pg.61]

However, even if this approach is regarded as giving a satisfactory account of chemical structure, it still remains to j ustify by full quantum mechanical means the treatment of the nuclei that it involves. But at present such a justification still eludes us. It may be in the future that the multiple well approach to nuclear permutational symmetry will be shown to be properly founded and thus the eigenvalues of the molecular Hamiltonian to be just those anticipated from the previous approach even so one will stUl be left with eigenfunctions which exhibit full permutation and rotation-inversion symmetry and it seems impossible to anticipate anything at aU like classical chemical structure from these using the standard quantum mechanical machinery. [Pg.53]

Figure 16-10. Potential energy (per phenyl-phenyl bond) for rotation in the terphcnyl molecule1 shown ( R = H, R=OCHj, R=C2H5). The central ring was rotated and subsequently the geometry was fully optimized while retaining inversion symmetry for the molecule. Figure 16-10. Potential energy (per phenyl-phenyl bond) for rotation in the terphcnyl molecule1 shown ( R = H, R=OCHj, R=C2H5). The central ring was rotated and subsequently the geometry was fully optimized while retaining inversion symmetry for the molecule.
D = dihedral (rotation plus dihedral rotation axes) I = inversion symmetry T = tetrahedral symmetry O = octahedral S5mimetry... [Pg.53]

In the Hermann-Mauguin Symbols, the same rotational axes are indicated, plus any inversion symmetry that may be present. The numbers indicate the number of rotations present, m shows that a mirror symmetry is present and the inversion symmetry is indicated by a bar over the number, i.e.- 0. [Pg.53]

It can be seen that there are seven other symmetry operations (roto-reflections) of this class, which is then denoted by SSe, the subscript 6 indicating a rotation through lit 16. In a similar way, we can analyze other symmetry operations of classes 65 4,15 2 (commonly called an inversion symmetry operation and denoted by /), and IE (the identity operation that leaves the octahedron unchanged). [Pg.239]

Figure 7.4 The effect of different symmetry operations over the three p orbitals (a) the initial positions (b) after an inversion symmetry operation (c) after a reflection operation through the x-y plane (d) after a rotation Cj about the z-axis. Figure 7.4 The effect of different symmetry operations over the three p orbitals (a) the initial positions (b) after an inversion symmetry operation (c) after a reflection operation through the x-y plane (d) after a rotation Cj about the z-axis.
Similarily, the 4,14-dicarboxylic acid 56 with C2-symmetry could also be resolved via its 1-phenylethylamine salts and its configuration unambiguously correlated with the monocarboxylic acid 55 through the monobromo derivative 5878). Accordingly 55 and 56 with the same sign of optical rotation have the same chirality. Many racemic and optically active homo- and heterodisubstituted 4,12- and 4,14-disubstituted [2.2]metacyclophanes have been prepared and chemically correlated 78,79) mainly to study their chiroptical properties78). Whereas 4,12-homodisubstituted compounds have a center of inversion ( -symmetry) and are therefore achiral meso-forms , the corresponding 4,14-isomers are chiral with C2-symmetry. All heterodisubstituted products are chiral (Q-symmetry see also Section 2.9.4 for the discussion of their chiroptical properties and their use as models for the application of the theory of chirality functions). [Pg.42]

Thus far we have addressed the symmetry of crystalline arrays only in terms of the proper rotations and the rotation-inversion operations (the latter including simple inversion, as 1, and reflection, as 2) that occur in point symmetries, along with the lattice translation operations. However, for a complete discussion of symmetry in crystalline solids, we require two more types of operation in which translation is combined with either reflection or rotation. These are, respectively, glide-reflections (or, as commonly called, glides) and screw-rotations. [Pg.384]

The first is Coov> which has a principal axis about which any rotation is a symmetry operation, plus an infinity of vertical planes containing the principal axis. Systems that in addition have inversion symmetry belong to D h-... [Pg.102]

The symmetry elements, proper rotation, improper rotation, inversion, and reflection are required for assigning a crystal to one of the 32 crystal systems or crystallographic point groups. Two more symmetry elements involving translation are needed for crystal structures—the screw axis, and the glide plane. The screw axis involves a combination of a proper rotation and a confined translation along the axis of rotation. The glide plane involves a combination of a proper reflection and a confined translation within the mirror plane. For a unit cell... [Pg.10]

Since the Laplacian V2 is invariant under orthogonal transformations of the coordinate system [i.e. under the 3D rotation-inversion group 0/(3)], the symmetry of the Hamiltonian is essentially governed by the symmetry of the potential function V. Thus, if V refers to an electron in a hydrogen atom H would be invariant under the group 0/(3) if it refers to an electron in a crystal, H would be invariant under the symmetry transformations of the space group of the crystal. [Pg.15]

FIGURE 4.6. A rotatory-inversion axis involves a rotation and then an inversion across a center of symmetry. Since, by the definition of a point group, one point remains unmoved, this must be the point through which the rotatory-inversion axis passes and it must lie on the inversion center (center of symmetry). The effect of a fourfold rotation-inversion axis is shown in two steps. By this symmetry operation a right hand is converted to a left hand, and an atom at x,y,z is moved to y,—x,—z. (a) The fourfold rotation, and (b) the inversion through a center of symmetry. [Pg.113]

The fourth type of symmetry operation combines rotational symmetry with inversion symmetry to produce what is called a rotatory-inversion axis, designated n (Figure 4.6). It consists of rotation about a line combined with inversion about a specific point on that line. For example, the operation of fourfold rotation-inversion is done by rotating an object at x,y,z through an angle of 90° about the z axis to produce an... [Pg.114]

By exploring the space inversion symmetry of the rotational basis functions, we can construct the parity-adapted rotational basis functions... [Pg.287]

Four simple symmetry operations - rotation, inversion, reflection and translation - are visualized in Figure 1.7. Their association with the corresponding geometrical objects and symmetry elements is summarized in Table 1.2. [Pg.10]


See other pages where Rotational inversion symmetry is mentioned: [Pg.126]    [Pg.126]    [Pg.596]    [Pg.172]    [Pg.405]    [Pg.610]    [Pg.752]    [Pg.704]    [Pg.62]    [Pg.285]    [Pg.161]    [Pg.496]    [Pg.388]    [Pg.244]    [Pg.245]    [Pg.247]    [Pg.249]    [Pg.631]    [Pg.53]    [Pg.198]    [Pg.13]    [Pg.147]    [Pg.50]    [Pg.48]    [Pg.55]    [Pg.250]    [Pg.42]    [Pg.151]   
See also in sourсe #XX -- [ Pg.250 ]

See also in sourсe #XX -- [ Pg.250 ]




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Inversion symmetry

Inversion symmetry of rotational levels

Inversion-rotation symmetry

Rotation symmetry

Rotation-inversion

Symmetry axis rotation-inversion

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