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Extinction band

When a nanoporous Ti02 film consisting of Ti02 nanoparticles is used instead of the single crystal, the extinction band of silver nanoparticles deposited by UV-irradiation is much broader. This is probably because the nanopores in the Ti02 film mold the silver nanoparticles into various anisotropic shapes [9], although direct observation of the particles in the nanopores is difficult. [Pg.264]

Localized plasmon resonance on noble metal nanostructures Noble metal nanostructures exhibit a strong UV visible extinction band with its peak position affected by the dielectric constant and thickness of the material surrounding the nanostructures 7,11 13... [Pg.78]

Convergent (or focused) beam electron diffraction (CBED) is particularly attractive for determining local crystal structures and space groups in three dimensions (Steeds et al 1979, Tanaka et al 1985). In a modern TEM, CBED is now routinely available. In this technique, two principles of TEM electron diffraction are employed departure from Friedel s law and the formation of extinction bands within refiections that are forbiddden by space groups. [Pg.61]

Calculations for a range of particle sizes are shown in Fig. 11.13. Note that the scales have not been shifted for the different sizes extinction increases with size because of scattering. The extinction band for the 0.1-jam particle faithfully reflects the characteristics of the intrinsic absorption band. But asymmetries develop for particles larger than about 0.2 jam indeed, at a radius of 0.3 jam the absorption band looks like an emission band relative to the continuum. The explanation for this strange extinction behavior near an absorption band lies in the preceding section extinction is not a steadily increasing function of bulk absorption. A narrow absorption band is similar to a small absorption edge that falls just as rapidly as it rises, which can thus cause extinction peaks, dips, or both. [Pg.308]

Of more recent discovery are wide and shallow extinction bands with characteristic widths of about 500-1000 A and extending from about 3400 to 11,000 A (for a brief survey, see Huffman, 1977). This very broad structure (VBS) is too broad and weak to be seen in Fig. 14.4. Lack of correlation between the diffuse bands and the VBS suggests a different origin for the two. [Pg.460]

With improved possibilities for infrared spectroscopy, broad extinction bands around 9.7 pm and 18 pm have been detected, which were ascribed to the stretching (Woolf Ney 1969) and bending (Treffers Cohen 1974) modes in the SiC>4 tetrahedron forming the building block of silicates, because they correspond to known absorption bands seen in all terrestrial silicates. These bands are also seen in the emission from dust shells around O-rich stars. This gave the first observational hints on the mineralogy of the silicate dust. The smooth, structureless nature of the bands indicated that the silicates in the ISM and in circumstellar dust shells are amorphous. [Pg.30]

From Eq. (4), it may be deduced that extinction bands will be observed for two different conditions ... [Pg.259]

Tordella [35] was probably the first to show HDPE and LDPE birefnngence patterns highly perturbed after the onset of flow instabilities. Discontinuities in the extinction bands and non stationary patterns were then observed, which was confirmed later by Vinogradov et al. [24] on polybutadienes or Oyanagi et al. [36] on HDPE and PS. Piau et al. [17] observed on polybutadiene slight pulsations at the die exit, correlated to the frequency of the sharkskin defect. [Pg.280]

When liquid crystalline specimens are viewed between crossed polars, it is the positions of extinction bands, and how the positions change as the crossed polars are rotated, that is used to find the point-to-point variation in molecular orientation. It is appropriate to examine the principles on which this analysis is based ... [Pg.243]

AuNPs in Liquid-State Environment Solute pure and monolayer-coated ( capped ) AuNPs are central targets in colloid and surface science also with a historical dimension [258-262]. Facile chemical syntheses introduced by Schmid et al. [260] and by Brust et al. [263] have boosted AuNP and other metal nanoparticle science towards characterization of the physical properties and use of these nanoscale metallic entities by multifarious techniques and in a variety of environments. Physical properties in focus have been the surface plasmon optical extinction band [264—269], scanning and transmission electron microscopy properties, and electrochemical properties of surface-immobilized coated AuNPs [173, 268-276], To this can be added a variety of AuNP crosslinked molecular and biomolecular... [Pg.120]

One way is to form the extinction bands by generation of colloidal silver via... [Pg.479]

After thermal decomposition of AgN3, Bartlett et al. [98] observed only one optical extinction band with unpolarized light at 490 nm, in agreement with... [Pg.319]

Figure 4.1 shows extinction spectra for spherical gold nanoparticles, with diameters of 20 and 100 nm, suspended in water. Gold nanoparticles with diameters of 20 and 100 nm exhibit broad extinction bands near 520 and 580 nm, respectively. Spectral features of the particles are well reproduced by Mie theory (Fig. 4.1b), and the bands are assigned to plasmon resonances. As mentioned, Mie theory gives rigorous solutions for spherical nanoparticles, and thus discrepancy between the observation and... [Pg.131]

Extinction spectra of single silver nanodisks have been reported [49]. The spectra shows an extinction band in the visible to near-infrared region that shifts toward the longer wavelength with the increment of the aspect ratio defined as (diameter)/(thickness), similar to the gold nanorods. The spectral bandwidth is broader than the gold nanorods. Since the sample is a single nanoparticle, the broad... [Pg.132]

Figure 5.205 Degree of crystallization (ratio of extinction bands E,2oo/Eu8o) oxidation... Figure 5.205 Degree of crystallization (ratio of extinction bands E,2oo/Eu8o) oxidation...
Figure 3.67 Polarized optical micrograph of a doubly banded spherulite in the chiral polymer poly(R-3-hydroxybutyrate). Two closely spaced extinction bands are separated by a wider light region the crystal strncture is orthorhombic and the indicatrix is an ehipsoid with two optic axes. Close inspection of the vertical arms of the Maltese cross reveals dark bands crossing the light regions from left to right, indicating that the twist is left handed. Scale bar is 25 mm. From Saracovan et al. [102] with permission from the American Chemical Society. Figure 3.67 Polarized optical micrograph of a doubly banded spherulite in the chiral polymer poly(R-3-hydroxybutyrate). Two closely spaced extinction bands are separated by a wider light region the crystal strncture is orthorhombic and the indicatrix is an ehipsoid with two optic axes. Close inspection of the vertical arms of the Maltese cross reveals dark bands crossing the light regions from left to right, indicating that the twist is left handed. Scale bar is 25 mm. From Saracovan et al. [102] with permission from the American Chemical Society.

See other pages where Extinction band is mentioned: [Pg.279]    [Pg.42]    [Pg.307]    [Pg.318]    [Pg.324]    [Pg.459]    [Pg.464]    [Pg.279]    [Pg.279]    [Pg.329]    [Pg.284]    [Pg.317]    [Pg.76]    [Pg.193]    [Pg.176]    [Pg.344]    [Pg.545]    [Pg.253]    [Pg.255]    [Pg.258]    [Pg.237]    [Pg.271]    [Pg.222]    [Pg.269]    [Pg.132]    [Pg.133]    [Pg.15]    [Pg.41]    [Pg.109]    [Pg.239]    [Pg.139]    [Pg.277]   
See also in sourсe #XX -- [ Pg.259 , Pg.280 ]




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Extinction

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