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Clusters four shell

The next available full-shell cluster that has been investigated by MoBbauer spectroscopy was the four-shell cluster Pt309phen 3603o+io (phen = 4,7-p-C6H4S03Na substituted 1,10-phenanthroline) [17]. Its inner core consists of 147 atoms. However, since platinum is not MoBbauer-active, the cluster sample had to be irradiated with thermal neutrons to transfer a fraction of the Pt... [Pg.8]

The next smaller ligand-protected nanocluster that was investigated by scanning tunneling spectroscopy (STS) was the four-shell cluster Pt309phen 36O20 [20,21]. The diameter of the Pt core is 1.8 nm, about a tenth of the former example. However, even here a Coulomb blockade could only be observed at 4.2 K, i.e. at room temperature the particle still has metallic behaviour. Since... [Pg.9]

It should be mentioned that corresponding investigations of slightly larger particles, for instance, of a Pt309 four-shell cluster with a 1.8 nm metal core, clearly indicated... [Pg.5942]

Figure 6.43 (a) A ball-and-stick view of the cationic cluster of [Eu54Ni54(IDA)4g (0H)i44(C03)6(H20)25] and (b) a four-shell presentation showing only its metal frameworks [25]. (Reproduced from Z.P. Zheng, Cluster compounds of the f-elements, in K.A. Gschneidner, Jr., J.C.G. Bilnzli, and V.K. Pecharsky (eds.). Handbook on the Physics and Chemistry of Rare Earths, volume 40, 2010, with permission from Elsevier.)... [Pg.263]

Kong, X., Ren, Y, Chen, W., Long, L., Zheng, Z., Huang, R. etal. (2008) A four-shell nesting doll-hke 3d-6f cluster containing 108 metal ions. Angewandte Chemie International Edition, 47, 2398—2601. [Pg.272]

The reconstruction of the f.c.c. Cu spectrum has been made by theoretical multiple scattering calculations. A quite good agreement with experiment is obtained with a four-shell 54-atom cluster, organized with 12 atoms at 2.55 A, 6 at 3.61 A, 24 at 4.42 A and 12 at 5.09 A. The four peaks of the spectrum are only reproduced when the third shell, at 4.42 A, is included. The reconstruction of a-Mn spectrum was not realized as either a b.c.c. or a f.c.c. packing lead to a good fit. [Pg.25]

In Fig. 20 the experimental Cu K-edge XANES is reported in the upper part of the figure. The multiple scattering calculations for copper clusters of different size are reported, in the lower part The calculations began with a simple cluster including only first neighbors (curve a), and then two shells (curve b), three shells (curve c) and four shells (lower curve) were included. [Pg.56]

Fig. 20. K edge XANES spectrum of Cu. The experimental spectrum (upper curve) is compared with multiple scattering calculation for different cluster sizes a) one shell b) two shells c) three shells and d) four shells... Fig. 20. K edge XANES spectrum of Cu. The experimental spectrum (upper curve) is compared with multiple scattering calculation for different cluster sizes a) one shell b) two shells c) three shells and d) four shells...
The quantitative aspect of the EXAFS technique is also well known and the literature gives several studies where chemisorption and EXAFS measurements are compared (see for example We can illustrate this particular contribution of the spectroscopy by a study of rare earth transition metal catalysts prepared from intermetallic LaNij-type compounds. The three classical preparation steps are here skipped with a carbon monoxide hydrogenation reaction. The intermetallic phase is transformed into a rare earth oxide upon which the transition metal is left as metallic clusters which form the active species. This transformation has been followed as a function of the time reaction In Fig. 5 we plot the Fourier transforms of CeNij at the nickel edge before the reaction (a), after 10 hours (b) and after 27 hours (c) under the CO + H2 mixture. These are all compared to elemental nickel (d). The increase of the amplitude of the first peak and the growth of three new ones at greater distances are the consequence of the formation of nickel particles. A careful analysis of these four shells has allowed us quantitatively to estimate the fraction of extracted nickel during the reaction as 30% after 10 hours and 80% after 27 hours on a CO + flux at 350 °C. [Pg.75]

A giant heterometallic cluster with its 108 metal ions organized into a four-shell Russian doll-like structure has been reported recently (Kong... [Pg.201]

FIGURE 97 A ball-and-stick view of the cationic cluster [Eu54Ni54(IDA)48(OH)i44 (C03)6(H20)2s] (left) and a four-shell presentation showing only its metal frameworks (right) (redrawn after Kong et al., 2008a). [Pg.202]

The four-shell, nesting doll-like structure of the cationic cluster is shown on Eigure 97. Moving outward, the irmermost shell (Shell 1)... [Pg.202]

Figure 3.107 TEM images of full-shell clusters, (a) A Pt309 four-shell cluster (b) A Pdsgi five-shell cluster. Figure 3.107 TEM images of full-shell clusters, (a) A Pt309 four-shell cluster (b) A Pdsgi five-shell cluster.
The presence of a compact inner-four-shell NH4 (NH3)4 is also suggested by enthalpy measurements for the clustering reactions NH4+(NH3) i + NH3 = NH4 (NH3) shown in Table V, in which a sharp drop off between AH4 3 and AH5 4 is observed. [Pg.351]

Figure 3-32. High resolution transmission electron micrograph of a four shell Pt309 cluster in the [110] direction. As in the bulk, the Pt atoms form a cubic close packed structure. Diameter L8 nm. Figure 3-32. High resolution transmission electron micrograph of a four shell Pt309 cluster in the [110] direction. As in the bulk, the Pt atoms form a cubic close packed structure. Diameter L8 nm.
A plot of the raw data and the best fit in k and R space for the wider range has been included in Fig 5. The first peak in the Fourier transform may be attributed to the six Ti-0 bonds of the basic octahedron, as already predicted from the XANES data. The distance is the same that the short bond of the distorted octahedra in anatase. The peaks between 3 and 6 A are a complex result of the overlap of four different features. The first one, Ti-Ti at 3.09 A, is very similar to the distance observed in anatase between two octahedra sharing edges (3.04 A), while the next one, Ti-O at 3.78 A, is very close to the distance of the oxygen atoms in the second octahedron (3.86 A). The shell Ti-0 would correspond to oxygen atoms in a third octahedron in an anatase-like structure. The shell Ti-0 has no correspondence in a cluster of anatase structure including four octahedra. In relation with the similarities with the anatase strucutre in the other four shell, it has to be pointed out the low coordination number of the Ti-Ti bond at 3.09 A, as well as the lack... [Pg.633]

When water undergoes self-ionization, a range of cationic species are formed, the simplest of which is the hydronium ion, HjO (Clever, 1963). This ion has been detected experimentally by a range of techniques including mass spectrometry (Cunningham, Payzant Kebarle, 1972), as have ions of the type H+ (HaO) with values of n up to 8. Monte-Carlo calculations show that HjO ions exist in hydrated clusters surrounded by three or four water molecules in the hydration shell (Kochanski, 1985). These ions have only a short lifetime, since the proton is highly mobile and may be readily transferred from one water molecule to another. The time taken for such a transfer is typically of the order of 10 s provided that the receiving molecule of water is correctly oriented. [Pg.44]

Completely closed, convex, single-shell clusters are called closo clusters their atoms form a polyhedron. If the polyhedron has only triangular faces, it is also called a delta-hedron. Depending on the number of available electrons, we can distinguish four general bonding types for closo clusters ... [Pg.139]

Other studies conducted on mixed protonated clusters of ammonia bound with TMA showed that the ion intensity distributions of (NH3)n(TMA)mH+191 display local maxima at (n,m) = (1,4), (2,3), (2,6), (3,2), and (3,8). Observation that the maximum ion intensity occurs at (n,m) = (1,4), (2,3), and (3,2) indicates that a solvation shell is formed around the NHJ ion with four ligands of any combination of ammonia and TMA molecules. In the situation where the maximum of the ion intensity occurs at (n,m) = (2,6) and (3,8), the experimental results suggest that another solvation shell forms which contains the core ions [H3N-H-NH3]+ (with six available hydrogen-bonding sites) and [H3N-H(NH2)H-NH3]+ (with eight available hydrogen-bonding sites). The observed metastable unimolecular decomposition processes support the above solvation model. [Pg.245]


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