Fabrication of devices from inorganic nanocrystals normally requires that they are self-organized into ordered structures. It has now been demonstrated that nanocrystals are able to self-organize in a 'supra'-crystal with a face-centred cubic (f.c.c.) structure. The physical properties of nanocrystals self-organized into compact arrays are quite different from those of both isolated nanocrystals and the bulk phase. The collective optical and magnetic properties of these nanocrystal assemblies are governed mainly by dipolar interactions. Here, we show that nanocrystals vibrate coherently when they are self-organized in f.c.c. supra-crystals. Hence, a phase relation exists between the vibrations of all of the nanocrystals in a supra-crystal. This vibrational coherence can be observed by a substantial change of the quadrupolar low-frequency Raman scattering peak. Although a change in electronic transport properties has previously been observed on self-organization of silver nanocrystals, vibrational coherence represents the first intrinsic property of f.c.c. supra-crystals.

The present study combines both experiment and molecular dynamics simulations in order to document the ionization behavior of the C 6 H 6 -H 2 O and C 6 H 6 -D 2 O complexes close to the ionization threshold, in particular its nonadiabatic character. Using the two-color two-photon resonant ionization laser technique, the ionization thresholds of these species have been measured together with the threshold for dissociative ionization. A binding energy has been deduced for the neutral species: D 0 (C 6 H 6 -H 2 O) ) 106 ( 4 meV and D 0 (C 6 H 6 -D 2 O) ) 116 ( 5 meV, which significantly increases the precision compared to literature. Using a semiempirical potential model, the minimum energy structures of the neutral and ionic species have been determined, and the potential energy surfaces have been analyzed using a two-dimensional approach. As a result, the formation of a stable C 6 H 6 + -H 2 O complex close to the threshold is found to be controlled by a pure quantum effect and is ascribed to the classically forbidden region of the neutral ground state wave function for the intermolecular vibrational motion. Using classical molecular dynamics simulations in order to sample this region, it has been shown that the neutral conformations involved in the production of stable ions at the ionization threshold exhibit a strong geometry change compared to the neutral equilibrium conformation; i.e., the water molecule is strongly shifted off the benzene C 6 axis and is also flipped over backward the benzene ring. The difference in the ionization energy of the C 6 H 6 -H 2 O and C 6 H 6 -D 2 O complexes, which cannot be explained by the difference in the neutral binding energies alone, supports this result.

Galvanic replacement reactions provide an elegant way of transforming solid nanoparticles into complex hollow morphologies. Conventionally, galvanic replacement is studied by stopping the reaction at different stages and characterizing the products ex situ. In situ observations by liquid-cell electron microscopy can provide insight into mechanisms, rates and possible modifications of galvanic replacement reactions in the native solution environment. Here we use liquid-cell electron microscopy to investigate galvanic replacement reactions between silver nanoparticle templates and aqueous palladium salt solutions. Our in situ observations follow the transformation of the silver nanoparticles into hollow silverpalladium nanostructures. While the silver-palladium nanocages have morphologies similar to those obtained in ex situ control experiments the reaction rates are much higher, indicating that the electron beam strongly affects the galvanic-type process in the liquid-cell. By using scavengers added to the aqueous solution we identify the role of radicals generated via radiolysis by high-energy electrons in modifying galvanic reactions.

Nanocrystal organizations represent a new generation of materials with specific properties compared with those of isolated nanocrystals and of the bulk material. Here, we present the first intrinsic crystalline growth properties of highly ordered mono- and multilayers of 5 nm silver nanocrystals. Triangular single crystals with face-centred-cubic structures are obtained by annealing the ordered nanocrystals under atmospheric pressure at 50 degrees C. The triangles are mixed with well-crystallized coalesced particles of various shapes. Their size depends on the initial nanocrystal ordering range on the substrate, which is local on amorphous carbon and highly extended on highly oriented pyrolitic graphite (HOPG). Hence, the single-crystal size is larger on HOPG than on amorphous carbon. These observations show that the crystalline growth properties of silver nanocrystals can be tailored by controlling their organization. Furthermore, on HOPG an epitaxial orientation of the triangles is observed.

The present study combines both experiment and molecular modeling to describe the photoionization behavior of the gas-phase hydrogen-bonded complexes of phenol with water, methanol, and dimethyl ether, in particular the occurrence of fragmentation following ionization. Using the two-color two-photon resonant ionization laser technique, the threshold for dissociative ionization of these species has been measured. For the first time, precise binding energies have been deduced for the neutral species: D 0(phenol−H2O) = 243 ± 5 meV and D 0(phenol−CH3OH) = 265 ± 8 meV. Using a semiempirical potential model, the minimum energy structures of both neutral and ionic species have been determined. This theoretical study has emphasized the role of the dispersive interactions in the geometry of these neutral complexes, in particular the interactions between the alkyl group of the solvent molecule (CH3 in the case of methanol or dimethyl ether) and the π-cloud of the aromatic molecule. In addition, the comparison between the neutral and ionic geometry of these complexes has allowed us to account qualitatively for the changes in the ionization properties within the complex series, namely in their zero kinetic-energy photoelectron spectra.

In this paper we describe collective properties of silver nanoparticles organized in two-dimensional superlattices. Our aim is to show that we can control the state of organization of the silver particles deposited on the substrate. Then the particles are found in the form of either a well-organized two-dimensional array of isolated particles or disordered and coalesced particles distributed more or less randomly on the surface. The optical spectra are compared with both polarized and unpolarized light. When particles are arranged in a hexagonal array, an asymmetrical and broad peak is observed. Under p-polarized light, a new high-energy peak appears that is interpreted as a collective effect, resulting from the mutual interactions between particles. We support this conclusion from numerical calculations performed on finite-size clusters of silver spheres, where only the electrodynamic interactions between the spheres are taken into account. With disordered and coalesced system the high-energy peak disappears whereas a peak toward low energy is observed. This is attributed to coalesced particles. ͓S0163-1829͑99͒12415-9͔

Here, we report a new synthetic route for spherical small copper nanoparticles (CuNPs) with size ranging from 3.5 nm to 11 nm and with an unprecedented associated monodispersity (<10%). This synthesis is based on the reduction of an organometallic precursor (CuCl(PPh3)3) by tert-butylamine borane in the presence of dodecylamine (DDA) at a moderate temperature (50 to 100 °C). Because of their narrow size distribution, the CuNPs form long-range 2D organizations (several μm(2)). The wide range of CuNPs sizes is obtained by controlling the reaction temperature and DDA-to-copper phosphine salt ratio during the synthesis process. The addition of oleic acid (OA) after the synthesis stabilizes the CuNPs (no coalescence) for several weeks under a nitrogen atmosphere. The nature and the reactivity of the ligands were studied by IR and UV-visible spectroscopy. We thus show that just after synthesis the nanoparticles are coated by phosphine and DDA. After adding OA, a clear exchange between phosphine and OA is evidenced. This exchange is possible thanks to an acid-base reaction between the free alkylamine in excess in the solution and OA. OA is then adsorbed on the NPs surface in the form of carboxylate. Furthermore, the use of oleylamine (OYA) instead of DDA as the capping agent allows one to obtain other NP shapes (nanorods, triangles and nanodisks). We get evidence that OYA allows the selective adsorption of chloride ions derived from the copper precursor on the different crystallographic faces during the growth of CuNPs that induces the formation of anisotropic shapes such nanorods or triangles.

By shortening solid-state diffusion times, the nanoscale size reduction of dielectric materials -such as ionic crystalshas fueled synthetic efforts towards their use as nanoparticles, NPs, in electrochemical storage and conversion cells. Meanwhile, there is a lack of strategies able to image the dynamics of such conversion, operando and at the single NP level. It is achieved here by optical microscopy for a model dielectric ionic nanocrystal, a silver halide NP. Rather than the classical core-shrinking mechanism often used to rationalize the complete electrochemical conversion and charge storage in NPs, an alternative mechanism is proposed here. Owing to its poor conductivity, the NP conversion proceeds to completion through the formation of multiple inclusions. The super-localization of NP during such heterogeneous multiple-step conversion suggests the local release of ions, which propels the NP towards reacting sites enabling its full conversion.