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Reflection respect

There are a number of reasons why the XRD peaks of LDH samples are often rather broad. The relatively small domain size, particularly in the (00/) direction, leads to line broadening. The Scherrer equation may be used to estimate the domain size in the a and c directions from the width of the (110) and (00/) reflections, respectively [119,120], although the inherent approximations in this method should always be borne in mind [121,122]. [Pg.20]

Fig. 9 Rietveld refinement of incommensurate Te-III at 8.5 GPa. The upper and lower tick marks below the profile mark the peak positions of the main and first order satellite reflections, respectively. The reflections shown in Fig. 8 are identified by their (hklm) indices, where the main reflections are indexed (M/O)... Fig. 9 Rietveld refinement of incommensurate Te-III at 8.5 GPa. The upper and lower tick marks below the profile mark the peak positions of the main and first order satellite reflections, respectively. The reflections shown in Fig. 8 are identified by their (hklm) indices, where the main reflections are indexed (M/O)...
Fig. 6 a TEM images of the CNT-g-P2VP after deposition of PB2 clusters. b,c HR TEM images of the core-shell structure of the particles consisting of a dense crystalline core (diameter of 3-5 nm) surrounded by a few nanometer-thick amorphous shell. HR TEM image (d) and selected area diffraction pattern (e) confirm the crystalline structure of the PB clusters (lattice distances of 2.09 A (Fe —N), 1.96 A and 1.83 A (Fe —C) that correspond to the (422), (333) and (404) reflections, respectively)... [Pg.166]

Figure 8.30. Antiphase domain boundaries in synthetic anorthite (Anioo). (a) Difiraction pattern showing sharp a-, b-, c-, and -reflections, (b), (c), and (d) Antiphase domain boundaries imaged in DF with b-, c-, and -reflections, respectively. (From McLaren and Marshall 1974.)... Figure 8.30. Antiphase domain boundaries in synthetic anorthite (Anioo). (a) Difiraction pattern showing sharp a-, b-, c-, and -reflections, (b), (c), and (d) Antiphase domain boundaries imaged in DF with b-, c-, and -reflections, respectively. (From McLaren and Marshall 1974.)...
The XRD method can be successfully apply to detect the /-/" phase boundary by analysing the (112) and (400)/(004) reflections respectively at about 42 and 61-64 20 (Fig. 6.3.) [22,23], even though, due to the low intensity of these peaks, confirmation by using a synchrotron radiation or even neutron scattering source may be desirable [45,46]. Due to the low intensity of the conventional XRD technique to the oxygen atoms, the / -c phase transition is best detected by using... [Pg.229]

Absolute value of h, k, and / is assumed. Max h+k + I values are provided for each basis set reflection, respectively. [Pg.445]

Fig. 19 GIXRD data for F8BT with molecular weight 255 kg/mol (A-C) and with molecular weight of 9 kg/mol (D-F). (A and D) Pristine, (B and E) annealed to Tg and slowly cooled, and (C and F) annealed to Tm and slowly cooled. The inner and outer rings in (A) correspond to the (001) and (004) reflections, respectively. The most likely orientations of the polymers with respect to the substrate is shown in (G), with the jt-stacking direction indicated by arrows. Reprinted with permission from [77]. (2005) by the American Chemical Society... Fig. 19 GIXRD data for F8BT with molecular weight 255 kg/mol (A-C) and with molecular weight of 9 kg/mol (D-F). (A and D) Pristine, (B and E) annealed to Tg and slowly cooled, and (C and F) annealed to Tm and slowly cooled. The inner and outer rings in (A) correspond to the (001) and (004) reflections, respectively. The most likely orientations of the polymers with respect to the substrate is shown in (G), with the jt-stacking direction indicated by arrows. Reprinted with permission from [77]. (2005) by the American Chemical Society...
A widely used method is the separate handling of the left and the right peak moieties (split-Pearson VII or SP7). The peak heights and positions are taken as identical for both halves, but for half widths and slope parameters separate parameter sets are used i.e. two additional parameters per reflection, respectively parameter sets U,V,W and a,b,c for the left and right moieties each). [Pg.117]

It is interesting to check the presence of nickel compounds in the modified samples. The X-ray powder diffraction patterns (Fig. 2A and B) of sample 2 (NiO SP) and sample 4 (NiO/SP), in contrast to those of pure SAPO, exhibit pronounced changes in the signal at 20=43.3 and 50.7 degrees (CoKa radiation), which obviously correspond to the NiO (111) and (200) reflections, respectively. The XRD pattern of sample 3 (NiAc SP) does not indicate the presence of a NiO phase (Fig.20. Evidently, there are essential differences in the state of nickel in the samples investigated and elucidation of this problem needs additional data obtained by other methods. Special attention should be paid to sample 3 where no NiO has been f ound. [Pg.297]

In accord with eqs. 3.37 and 3.38 in the case of external excitation of the field, two shells are equivalent to one shell which has the following expressions for coefficient of screening and reflections, respectively ... [Pg.153]

Lipscomb 181) has presented a speculative discussion of the effects of pH on carboxypeptidase activity in relation to the high-resolution three-dimensional structures. In this interesting paper, Lipscomb proposes that the apparent pKa values observed in the pH profiles shown in Fig. 10 reflect respectively the ionization of Glu-270 (pKa 6.7) and the ionization of the zinc ion-coordinated water molecule (pKa 8.9). [Pg.113]

The large, asymmetric (Pi) unit cell permits 338 possible reflections in the angular range studied. Most peaks are composed of many unresolvable reflections. For instance, the major peaks at 12.3, 19.9, 22.0, and 1(0.8 (to which iTo, 110, 200, and 310, respectively, are the major contributors) contain 6, 9, 10 and i(0 reflections, respectively. In the Rietveld method, the intensity at any point in the calculated diffraction pattern is the sum of contributions from neighboring reflections. In the diffraction... [Pg.74]

Mention should also be made of signature adaptation that makes use of negative interference to reduce the probability of detection. In this case, the signature protective layer is adjusted so that negative interference occurs between the radar radiation that is reflected respectively from the outer surface and from the underlying metal, thus causing a black-out of the net reflection from the surface. The reflections in this case need to be adjusted so that 50% is reflected at the outer layer and 50% at the metal surface and so that the phase shift between these reflected radiations becomes half a wavelength at the outer surface. [Pg.568]

Fig. 4.15 A fibre pattern from a highly oriented sample of polyethylene. Note the two strong equatorial reflections very close together just over a third of the way out from the centre of the pattern shown. They are, from the centre outwards, the (110) and (200) reflections, respectively. (Courtesy of Dr A. P. Unwin.)... Fig. 4.15 A fibre pattern from a highly oriented sample of polyethylene. Note the two strong equatorial reflections very close together just over a third of the way out from the centre of the pattern shown. They are, from the centre outwards, the (110) and (200) reflections, respectively. (Courtesy of Dr A. P. Unwin.)...
The fibre pattern obtained for a particular sample of polyoxymethy-lene -fCH2—using X-rays of wavelength 0.154 nm exhibits equatorial reflections at angles of 21.9°, 37.7° and 23.2°. Show that these spots may be consistently indexed as the (110), (200) and (020) reflections, respectively, of an orthorhombic unit cell. The first layer line corresponds to the angle 25.6° and the unit cell contains four repeat units. Calculate the density of the crystalline material. [Pg.116]


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See also in sourсe #XX -- [ Pg.3 , Pg.50 , Pg.54 , Pg.57 , Pg.67 , Pg.67 , Pg.68 , Pg.77 ]




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