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Structure Image

Coating control and evaluation by the restitution of the coated structure image. [Pg.290]

In Fig. 4 we show an atomic resolution image of a carbon tube. The structure imaged at the upper right corner of the picture comes from another tube. Both of them were —1000 A long. A perfect honeycomb surface structure is observed. By taking into account the curvature of the tube surface and the STM imaging profile, we find the same lattice parameter as that of. graphite (1.42 A). This directly proves that the tubu-... [Pg.66]

TEM is still the most powerful technique to elucidate the dispersion of nano-filler in rubbery matrix. However, the conventional TEM projects three-dimensional (3D) body onto two-dimensional (2D) (x, y) plane, hence the structural information on the thickness direction (z-axis) is only obtained as an accumulated one. This lack of z-axis structure poses tricky problems in estimating 3D structure in the sample to result in more or less misleading interpretations of the structure. How to elucidate the dispersion of nano-fillers in 3D space from 2D images has not been solved until the advent of 3D-TEM technique, which combines TEM and computerized tomography technique to afford 3D structural images, incidentally called electrontomography . [Pg.543]

Figure 4, Area of benzene covered gold (111). surface, for two different objective len.s defooi a.s required for unique image interpretation (see 2 ). Tri a) the gold atomic columns are black, in b) white. Moire fringes, rather than any true structural image, result from the benzene monolayer. Simulations (right) have benzene overlay on top surface only. Figure 4, Area of benzene covered gold (111). surface, for two different objective len.s defooi a.s required for unique image interpretation (see 2 ). Tri a) the gold atomic columns are black, in b) white. Moire fringes, rather than any true structural image, result from the benzene monolayer. Simulations (right) have benzene overlay on top surface only.
Funami, T., Hiroe, M., Noda, S., Asai, I., Ikeda, S., and Nishinari, K. (2007). Influence of molecular structure imaged with atomic force microscopy on the rheological behavior of carrageenan aqueous system in the presence or absence of cations. Food Hydrocolloids 21, 617-629. [Pg.238]

Fig. 2. (a) Ray diagram in the electron microscope under imaging (microscopy) conditions. E electron source C condenser lens S sample O objective lens bfp back focal plane of O I intermediate lens P projector lens, (b) Structural imaging, diffraction and compositional functionalities of TEM. [Pg.202]

Fig. 3. HRTEM atomic structure image of germanium silicalite (GeSi04) in which there are channels of aperture diameter 0.55 nm running along the [010] direction. Inset shows the 5- and 6-membered smaller apertures that are circumjacent to larger (0.55 nm) channels (5). Fig. 3. HRTEM atomic structure image of germanium silicalite (GeSi04) in which there are channels of aperture diameter 0.55 nm running along the [010] direction. Inset shows the 5- and 6-membered smaller apertures that are circumjacent to larger (0.55 nm) channels (5).
Fig. 18. (a) Atomic structure image ofVPOand(b) electron diffraction (ED) at room temperature. [Pg.227]

Electron microscopy easily yields structural images of cast bilayer films. Figure 6 shows a scanning electron microscope (SEM) image of the cross section of the bilayer film of CgAzoCioN+Br prepared by the simple casting of water solution. From the presence of well developed layers parallel to die film plane, it can be assumed that the cast film was composed from multiple highly oriented bilayers. [Pg.57]

The transmission electron microscope is now well established as a useful tool for the characterization of supported heterogeneous catalysts(l). Axial bright-field imaging in the conventional transmission electron microscope (CTEM) is routinely used to provide the catalyst chemist with details concerning particle size distributions, 3), particle disposition over the support material(2-6) as well as particle morphology(7). Internal crystal structure(8-10), and elemental compositions(ll) may be inferred by direct structure imaging. [Pg.360]

Figure 2 Crystal structure of PKA and conserved active site, (a) Crystal structure image of PKA (green) in complex with peptide substrate inhibitor, ATP is displayed as a ball and stick structure (blue) and Mg + Ions (orange), (b) ATP binding residues of the kinase with ATP (blue), Mg + ions (orange), and substrate (red) are shown. Figure 2 Crystal structure of PKA and conserved active site, (a) Crystal structure image of PKA (green) in complex with peptide substrate inhibitor, ATP is displayed as a ball and stick structure (blue) and Mg + Ions (orange), (b) ATP binding residues of the kinase with ATP (blue), Mg + ions (orange), and substrate (red) are shown.
There are several disadvantages with the image simulation method. A nearly correct structure model is needed beforehand. This is often not available, especially for relatively complicated structures. Images are compared visually and no quantitative figure of merit is used for judging how well images and simulations agree. [Pg.8]

The projected potential is proportional to the negative of the image intensity, i.e. black features in HREM positives (low intensity) correspond to atoms (high potential). The corresponding image is called the structure image. [Pg.283]

MA O Keefe, P Buseck, S Ijima. Computed crystal structure images for high resolution electron microscopy. Nature 274 322 - 324, 1978. [Pg.298]

The fact that all deconvoluted images given in the middle row of Fig. 3 are very similar to one another in contrast and all metallic atoms are resolved as black dots with correct positions denotes that the image deconvolution technique is powerful to transform the image taken at an arbitrary defocus into the structure image. It is for the first time to clarify that the deconvoluted images still reveal the projected structure even if some reflections fall in the vicinity of zero cross of CTF. [Pg.536]

Greenhalgh, C., Cisek, R., Prent, N., Major, A., Aus der Au, J., Squier, J., and Barzda, V. 2005. Time and structural image analysis of microscopic volumes, simultaneously recorded with second harmonic generation, third harmonic generation, and multiphoton excitation fluorescence microscopy. Proc. SPIE 5969 59692F1-F8. [Pg.99]

Oron, D., Yehn, D., Tal, E., Raz, S., Fachima, R., and Silberberg, Y. 2004. Depth-resolved structural imaging hy third harmonic generation microscopy. J. Struct Biol. 147 3-11. [Pg.123]

Debarre, D., Pena, A. M., Supatto, W., Boulesteix, T., Simpler, M., Sauviat, M. R, Martin, J. L., Schanne-Klein, M. C., and Beaurepaire, E. 2007. Second- and third-harmonic generation microscopies for the structural imaging of intact tissues. Med. Sci. 22 845-50. [Pg.161]

In the following sections examples of applications of HREM structure imaging and high spatial resolution EDX microanalysis often from the same areas, to the hole superconductors are given. [Pg.566]

Figure 4 (a) Schematic of the perfect crystal structure of 123. (b) Schematic of a twin, (c) Low magnification TEM (diffraction contrast) image of twins observed on (110) planes, (d) HREM structure image of 123 in [010] at a defocus of -70 nm. Atoms are white and individual atom columns are shown. The corresponding selected area... [Pg.572]

E. M. Valera, S. V. Faraone, K. E. Murray and L. J. Seidman, Meta-analysis of structural imaging findings in attention-deficit/hjrperactivity disorder. Biol. Psychiatry, 2007, 61(12), 1361-1369. [Pg.150]


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