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Forbidden reflections

Assuming spherical symmetric charge densities, the fourth group is forbidden. Hence, these reflections provide information about the anisotropic copper displacement parameters and chemical bonding, and a correct determination of these forbidden reflections gives evidence of the data quality. [Pg.221]

Misorientation can be an issue during the time of collection of ED patterns as sometimes this can exceed 60 min in accumulation mode, and d5mamical diffraction contribution is observed (we may anticipate its presence due to the appearence of forbidden kinematically reflections in the pattern like +- 002). However, is important to note that misorientation effects become less critical and intensity of such forbidden reflections is lowered after applying precession mode to the ED pattern. Similar results have also been observed by M.Gemmi with Si samples. [Pg.180]

The contribution of harmonics is not normally large at first- and second-generation synchrotron sources, as the F i i value falls rapidly with increasing diffraction vector. A major exception is where weak quasi-forbidden reflections... [Pg.243]

For higher-order forbidden reflections, the bonding effects will be less and... [Pg.249]

Tischler, J. Z., Temperature Dependence of Higher Order Forbidden Reflections in Silicon and Germanium using Synchrotron Radiation, Thesis, Cornell University, Ithaca, NY (1983). [Pg.343]

Occasionally, reflections that are forbidden by the structure factor are observed in a diffraction pattern. These forbidden reflections are due to double diffraction, which occurs when a strong diffracted beam in the crystal acts as an incident beam for further diffraction by the crystal. These extra spots can be found by translating the diffraction pattern, without rotation, so that the 000 spot coincides successively with all the strong diffraction spots of the pattern. All new spots introduced by this procedure are geometrically possible double-diffraction spots. If A AT / and h2k2h are the indices of any two allowed primary diffraction spots, then all spots... [Pg.62]

Such an experiment is not easy to perform and is very time consuming because of the very small magnetic structure factors for the forbidden reflections. The investigation of MnF2 was important however, both in demonstrating the application of polarized neutron techniques to antiferromagnetic materials and in revealing directly the covalent spin density transferred to the fluorines [the existence of this spin density was already known of course, from NMR measure-... [Pg.70]

Calculated after Palatnik et al. Forbidden reflections in Fd3m... [Pg.204]

Bravais lattice Allowed reflections Extinct (forbidden) reflections... [Pg.224]

FIGURE 6 (a) Graphical construction for multiple diffraction on a square planar reciprocal lattice net.14 (b) Dependence, on rotation angle around die diffraction vector, of multiple reflection contribution to the apparent reflection intensity of 222, a forbidden reflection, in germanium.9 (c) Multiple reflection effects for several unrelated reflections, in rotation around the diffraction vector, showing peaks and dips. 1... [Pg.170]

Tilting experiments with the c -axis as tilt-axis have allowed determination of the reflection conditions in the [001] zone diffraction pattern. In Fig. 7.10 streaks at positions A -I-1, h- - and h- -, A -I-1 are systematically absent. Indexed with respect to the superstructure mesh one obtains streaks AO/ with A odd and Okl with k odd are absent. Reflection conditions in the plane thus become AO with A even and OA with k even. Note that double diffraction fills in the forbidden reflections in the [001] zone diffraction pattern. Knowledge of... [Pg.172]

The coherent position in this case is the averaged fractional d-spacing position of the two sites (Fig. 6). If the two equally occupied sites have a separation of exactly one-half of a -spacing along a particular , then = 0 for that particular this is analogous to a forbidden reflection in crystallography. [Pg.231]

The assumptions concerning the symmetry of the unit cell noted above have been the basis of recent refinements of the structure of cellulose I. In one such refinement (17) the forbidden reflections were simply assimed negligible, and the intensity data from Valonia cellulose were used to arrive at a final structure. In another study, the inadequate informational content of the diffractometric data was complemented with analyses of lattice packing energies (29) the final structures were constrained to minimize the packing energy as well as optimizing the fit to the diffractometric data. [Pg.6]

Experimental GISAXS pattern and indexations of a porous PFS template after removal of the minority component (a, d), nanostructured hydrated Ti(IV) oxide films with the PFS block still In place (b, e) and annealed titania network array (c, f). The patterns were analyzed using the distorted wave Born approximation to account for scattering of both the direct and reflected beam.S S5 and denote the diffraction peaks due to scattering of the direct and reflected X-ray beams, respectively. and indicate "forbidden" reflections. Only the diffraction peaks due to the direct beam scattering are indexed and only observed peaks are marked. Figure reproduced with permission from Ref. [61]. [Pg.93]

Attempts to determine experimentally the values of and Wm were carried out using various techniques internal friction [36,37], deformation under load pulse sequence [38], and TEM. There are very few internal friction experiments on semiconductors. The reason is the brittleness of these materials and the need to work at very low frequencies in order to get a relaxation peak at moderate temperatures. The direct observation of kink motion was realized by TEM, either by studying the relaxation of out-of-equilibrium dissociated dislocations [39], by in situ deformation [40], or by using forbidden reflections in the high-resolution mode [41,42]. These various experiments were analyzed within the framework of the kink-diffusion model of Hirth and Lothe [12], which does not take into account... [Pg.57]

Lattice fringes associated with these forbidden reflections have also been seen in high-resolution (HR) TEM studies, as have lattice spacing from other crystallographic faces [111, 116, 119]. In summary, whilst the (111) orientation of silver nanoprisms is generally accepted, the identity of the crystal faces at the edge of the nanoplates has yet to be confirmed. [Pg.133]


See other pages where Forbidden reflections is mentioned: [Pg.221]    [Pg.35]    [Pg.82]    [Pg.291]    [Pg.415]    [Pg.528]    [Pg.529]    [Pg.71]    [Pg.76]    [Pg.145]    [Pg.118]    [Pg.7]    [Pg.6029]    [Pg.63]    [Pg.70]    [Pg.71]    [Pg.30]    [Pg.39]    [Pg.409]    [Pg.516]    [Pg.531]    [Pg.124]    [Pg.6028]    [Pg.210]    [Pg.165]    [Pg.28]    [Pg.39]    [Pg.39]   
See also in sourсe #XX -- [ Pg.75 ]

See also in sourсe #XX -- [ Pg.249 ]

See also in sourсe #XX -- [ Pg.30 , Pg.39 ]

See also in sourсe #XX -- [ Pg.165 ]




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