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Restricted Symmetry

The symmetries for the seven basic crystal systems described above assume the full symmetry or holohedry of each of the lattices. When the basis is added, some of these symmetries may be restricted. For example, a face-centered cubic (fee) crystal such as A1 has the full cubic symmetry. However, diamond also has the fee structure with atoms occupying the lattice points as well as every other tetrahedral interstitial point. Its point group is 43m, which implies a rotation-inversion on the fourfold axes. The threefold symmetry is preserved without the threefold rotation-inversion. The twofold symmetry is no longer preserved and the only mirror symmetry is along the 110 planes. [Pg.72]

In another example, at temperatures 393 K, barium titanate has the perovskite structure, which is simple cubic with all of the symmetry elements of the cubic lattice, so its point group is Oh or m3m. As the temperature is reduced to its Curie temperature, the lattice contracts and the oxygen ions on the faces of the cube squeeze the titanium ion in the center of the cube so that it is displaced in one direction while the oxygen ions are displaced in the opposite direction, destroying the inversion symmetry as well as the mirror symmetry about the central plane and the rotational symmetry about several of [Pg.72]

Each of the other crystal systems has similar restricted symmetries and it can be shown that there is a total of 32 unique sets of point symmetry operations or point groups. The symmetry of every crystalline structure may be described by one of these 32 point groups. Such classification of point symmetries is useful in the search for materials with certain properties. For example, if one is looking for materials with permanent dipole moments, one would look only at systems that are noncentrosymmetric, i.e., systems that do not possess a center of inversion symmetry. The 10 noncentrosymmetric point groups are 1, 2, 3, 4, 6, m, 2mm, 3m, 4mm, and 6mm. [Pg.73]

Notice that rotation symmetry only exists for n = l, 2, 3, 4, and 6 five- and sevenfold rotations are not allowed because bodies with these symmetries cannot fill all space for the same reason that you cannot tile a floor with pentagons or with septagons. Icosahedral quasicrystals with fivefold symmetry can form, but cannot grow into crystalline solids in the strict sense of the word. Even so, such quasicrystals are extremely interesting both theoretically as well as from applications that utilize their unusual properties, as discussed later. [Pg.73]


Since the minimal basis model has only two basis functions with coefficients that can be varied and since molecular orbitals are constrained to be normalized, the minimal basis model has, in the general case, only one degree of freedom. An unrestricted solution, unlike the restricted solution, is not symmetry determined and a convenient way of incorporating this one degree of freedom into unrestricted calculations is to write the unrestricted occupied molecular orbitals and ij/ i as linear combinations of the restricted symmetry determined orbitals ij/i and 2 follows ... [Pg.222]

Structural restriction symmetry The number of carbon signals in a NMR spectrum can be prescribed, assuming sufficiently high spectrometer resolution. In this case the generator outputs only the structures with the prescribed number of classes of symmetry equivalent carbon atoms, based on topological symmetry. [Pg.182]

The close relation between the total s-electron density and the degree of covalent bonding is well characterized through the parallelism between I.S, and nephelauxetic effect (N.E.) (3), The partial occupation of the 4s orbitals and the bonding involving d electrons are included respectively in the central field CO valency and in the restricted symmetry covalency, which determine the N.E. (4). [Pg.5]

Other exceptions include polymers with restricted symmetry which can, however, erystallize in a helical macroconformation because of electrostatic interactions between molecular groups of the main chain ( intrachain interactions). However, for sueh helicity to occur, the chain should exhibit a great mobility, which is the ease, for example, in the family of polyethers in the latter case, the dipole attraetion due to —groups is responsible for the stability of the crystalline state poly(ethylene oxide) (-CH2-CH2-0-) crystallizes in a I2 helix (c = 1.94 nm), whereas poly(oxymethylene) (-CH2-0-) (also called polyformaldehyde or polyacetal ) does in a 9s helix (c = 1.72 nm). In the latter case, multiple dipole interactions contribute to stiffen the chains and enhance mechanical properties of the corresponding materials. [Pg.111]

The character tables of these groups are given in table Al.4.6 and table Al.4.71. If there were no restriction on pemuitation symmetry we might think that die energy levels of the H2 molecule could be of any one of the following four syimnetry... [Pg.173]

In the present calculations, the molecule is restricted to Cs symmetry. There are five internal degrees of freedom fthe out-of-plane mode is excluded to preserve C, symmetry). Nuclear configurations will be denoted R = (R(H -O). / (0-H ), / (h2-H ), corresponding to the... [Pg.465]

As we proceed to molecules of higher symmetry the vibrational selection rules become more restrictive. A glance at the character table for the point group (Table A.41 in Appendix A) together with Equation (6.56) shows that, for regular tetrahedral molecules such as CH4, the only type of allowed infrared vibrational transition is... [Pg.180]

One particularly important correlation is between 3aj and 1ti . Because of the relaxation of symmetry restrictions in the 2 compared with the point group, bending of the molecule results in some mixing between what become the 3aj and 2aj MOs. Since 2aj is strongly bonding, with considerable 2s character, one effect of the mixing is to impart some... [Pg.263]

Crystals A crystal may be defined as a solid composed of atoms arranged in an orderly, repetitive array. The interatomic distances in a ciyst of any definite material are constant and are characteristic of that material. Because the pattern or arrangement of the atoms is repeated in all directions, there are definite restrictions on the lands or symmetry that crystals can possess. [Pg.1653]

The same principal ideas are incorporated in the calculation protocols for symmetrical oUgomers as with asymmetrical systems, i.e., the weight is reduced specifically for ADRs or all distance restraints. In addition, the symmetry of the system restricts conforma-... [Pg.266]

The symmetry properties of an icosahedron are not restricted to the surface but extend through the whole volume. An asymmetric unit is therefore a part of this volume it is a wedge from the surface to the center of the icosahedron. Sixty such wedges completely fill the volume of the icosahedron. [Pg.328]

The lack of a well-defined specular direction for polycrystalline metal samples decreases the signal levels by 10 —10, and restricts the symmetry information on adsorbates, but many studies using these substrates have proven useful for identifying adsorbates. Charging, beam broadening, and the high probability for excitation of phonon modes of the substrate relative to modes of the adsorbate make it more difficult to carry out adsorption studies on nonmetallic materials. But, this has been done previously for a number of metal oxides and compounds, and also semicon-... [Pg.449]

The quantity x is a dimensionless quantity which is conventionally restricted to a range of —-ir < x < tt, a central Brillouin zone. For the case yj = 0 (i.e., S a pure translation), x corresponds to a normalized quasimomentum for a system with one-dimensional translational periodicity (i.e., x s kh, where k is the traditional wavevector from Bloch s theorem in solid-state band-structure theory). In the previous analysis of helical symmetry, with H the lattice vector in the graphene sheet defining the helical symmetry generator, X in the graphene model corresponds similarly to the product x = k-H where k is the two-dimensional quasimomentum vector of graphene. [Pg.40]

The singlet-level theory has also been used to describe the structure of associating fluids near crystalline surfaces [30,31,76,77]. The surface consists explicitly of atoms which are arranged on a lattice of a given symmetry. The fluid atom-surface atom potential can also involve an associative term, i.e., the chemical-type bonding of the adsorbate particles with the surface may be included into the model. However, we restrict ourselves to the case of a nonassociative crystalline surface first. [Pg.182]

For large this sum is again dominated by the first eigenvalue, Ai, which will now depend on M. For practical calculations M is restricted by computer memory. However, the symmetry of the Hamiltonian allows a block... [Pg.449]

Type II restriction enzymes have received widespread application in the cloning and sequencing of DNA molecules. Their hydrolytic activity is not ATP-depen-dent, and they do not modify DNA by methylation or other means. Most importantly, they cut DNA within or near particular nucleotide sequences that they specifically recognize. These recognition sequences are typically four or six nucleotides in length and have a twofold axis of symmetry. For example, E. coU has a restriction enzyme, coRI, that recognizes the hexanucleotide sequence GAATTC ... [Pg.351]

Table 11.5 lists many of the commonly used restriction endonucleases and their recognition sites. Because these sites all have twofold symmetry, only the sequence on one strand needs to be designated. [Pg.353]

The full Cl expansion within the active space severely restricts the number of orbitals and electrons that can be treated by CASSCF methods. Table 4.3 shows how many singlet CSFs are generated for an [n, n]-CASSCF wave function (eq. (4.13)), without any reductions arising from symmetry. [Pg.120]

In a general concept of a symmetry-restricted anharmonic theory Krumhansl relates the phonon anomalies to the electron band topology. The latter is directly determined by the competition of nearest neighbour interactions which in turn can be a function of stress, composition and temperature Nagasawa, Yoshida Makita simulated the <110> ... [Pg.329]

R.J. Gooding and I.A. Kmmhansl, Symmetry-restricted anharmonicities and the CsCl-to-7R martensitic... [Pg.332]


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Symmetry restrictions

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