Silver iodide nanowires grown within tubular J-aggregates.

Silver iodide nanowires have been grown within tubular J-aggregates of the cyanine dye 3,3'-bis(2-sulfopropyl)-5,5',6,6'-tetrachloro-1,1'-dioctylbenzimida-carbo-cyanine (C8S3) from aqueous AgNO3 solutions. Crystal structure analysis by selected area electron diffraction (SAED), high resolution transmission electron microscopy (HRTEM) and energy-dispersive X-ray spectroscopy (EDXS) of single nanowires revealed that they are of silver iodide (AgI), while previously they were presumed to be of metallic silver. Iodine has not been added intentionally, but it is a remnant from the chemical synthesis of the dye and present in a dye:iodine ratio of almost 2:1, as revealed by inductively coupled plasma mass spectrometry (ICP-MS). The AgI wires grow as single crystals with lengths of several 10-100 nm and width of 6.5 ±â€¯0.5 nm. The width and the orientation of the crystal relative to the aggregate axis are defined by the tubular structure of the templating dye aggregate. Caused by the nucleation at the tube wall the main growth is not along the usually preferred [0 0 0 1] direction but along the extension of the basal plane, which is furthermore tilted by an angle of 6°â€¯±â€¯2° against the main axis of the aggregate. This self-assembled system represents an organic-inorganic hybrid system with a well-defined semiconductor nanowire, AgI, that is strictly oriented with respect to the aggregated phase of conjugated molecules.

Rapid trench channeling of graphenes with catalytic silver nanoparticles.

We demonstrate trench channeling of mono- and multilayer graphenes with silver nanoparticles with high speed in ambient environment and at elevated temperatures. A silver nanoparticle located at a graphene edge catalyzes oxidation of neighboring carbon atoms, thereby burning a trench into the graphene layer. High-resolution scanning tunneling microscopy imaging reveals that the trench edges are very smooth with a peak-to-peak roughness below 2 nm. We discuss the channeling mechanism and demonstrate that channeling speeds of up to 250 nm/s and the smoothness of the resulting trenches indicate the prospect of a "catalytic pen" for high-precision lithography on graphenes.

Internal structure of nanoporous TiO2/polyion thin films prepared by layer-by-layer deposition.

The internal structure of porous TiO2 films prepared by electrostatic layer-by-layer deposition was investigated. The films were prepared by alternate dipping of solid substrates into dispersions of TiO2 nanoparticles and polycations, polyanions, or pure buffer solution, respectively. The surface charge of the amphoteric TiO2 particles was controlled by the pH of the aqueous dispersions. The morphology of the film surface was investigated by means of scanning electron microscopy. It was found that the surface roughness strongly depends on the polymeric material used for the deposition process but is independent of the ionic strength of the solution or the molecular weight of the polyions. The samples with rough surfaces feature strong light scattering. The porosity and internal structure of the TiO2/polyelectrolyte films were investigated by adsorption/desorption of dye molecules. A crude estimate yields an internal surface that is up to 160 times the plane surface of the substrate for a film thickness of 1 microm. The composition of the films was investigated by X-ray photoelectron spectroscopy (XPS). Detection of the XPS signal after each deposition step of the first three dipping cycles shows a significant increase of the relative surface coverage of Ti after the TiO2 deposition step and of PSS after the PSS deposition step. For later dipping cycles, such an increase was also detectable but less prominent.

Polarity of layer-by-layer deposited polyelectrolyte films as determined by pyrene fluorescence.

The polarity of polyelectrolyte (PE) multilayer films is investigated with pyrene as a polarity-sensitive probe. Multilayer films of poly(styrene sulfonate) (PSS) and various polycations were prepared by the layer-by-layer self-assembly technique. Pyrene (PY) molecules were inserted into the films by exposing the multilayers to pyrene solutions. By this method a homogeneous distribution of pyrene molecules at low concentration within the film was obtained. The ratio of the fluorescence intensities of the first (I) to the third (III) vibronic band (Py-value) of the pyrene emission spectrum is employed here to determine the polarity of the PE films. PSS and poly(allylamine hydrochloride) (PAH) multilayer films yielded a pyrene value close to the solvent polarity of acetone, while multilayers of PSS and poly(diallyldimethylammonium chloride) (PDADMAC) displayed a value higher than the one corresponding to water. The pyrene values of the polyelectrolyte films were independent from the solvent employed for probe dissolving. Although no direct relationship between solvent polarity and dielectric constant (epsilon) is available, an estimate of the static dielectric constant of the films can be provided by comparing the Py-values of the films with those of various solvents. Changes in the humidity conditions of the film environment in a closed cell did not affect the film polarity. However, a drastic and irreversible reduction of polarity could be induced by actively drying the samples by a nitrogen flow.

Genetic correlations between initial sensitivity to Ethanol and brain cAMP signaling in inbred and selectively bred mice.

BACKGROUND: Several lines of evidence have suggested a role for cAMP (adenosine 3',5'-cyclic monophosphate) signaling in the acute and chronic effects of ethanol. This study investigated whether there is a genetic correlation between cAMP synthesis in the brain and the acute effects of ethanol [alcohol sensitivity or acute functional tolerance (AFT)]. METHODS: By using nine inbred strains of mice, we measured initial sensitivity and AFT to ethanol with a test of balance on a dowel. Initial sensitivity was defined by the blood ethanol concentration (BEC0) at the loss of balance on a dowel after an ethanol injection [1.75 g/kg intraperitoneally (ip)]. When mice were able to regain balance on the dowel, BEC1 was determined, and a second ethanol injection was given (2 g/kg ip). Upon final regaining of balance, BEC2 was determined. AFT was defined by the difference between BEC1 and BEC2 (AFT = DeltaBEC = BEC2 - BEC1). Cyclic AMP synthesis was measured in whole-cell preparations in the cerebellum and other brain areas of mice of the nine inbred strains. RESULTS: Significant differences in BEC0 and AFT were seen among the mice of the nine inbred strains. Cerebellar basal and forskolin- and isoproterenol-stimulated cAMP production differed significantly between the strains, and BEC0 was found to correlate significantly with forskolin- and isoproterenol-stimulated cAMP accumulation in the cerebellum (r = 0.70 and 0.94, respectively). When we measured cAMP production in mesencephalic and telencephalic tissue in three strains of mice that differed significantly in isoproterenol-stimulated cAMP accumulation in the cerebellum, significant differences between strains were found only in telencephalic tissue. The relative relationship between the rank order of the three strains for cAMP accumulation in the telencephalon and initial sensitivity to ethanol was identical to that seen with the cerebellum. However, AFT did not correlate with cAMP accumulation in the cerebellum or any other brain area tested. CONCLUSIONS: These results suggest that cAMP-generating systems of the cerebellum and possibly the brain areas contained in telencephalic tissues (e.g., basal ganglia) may have an important relationship to an animal's initial sensitivity to the incoordinating effects of ethanol.

Chiral J-aggregates formed by achiral cyanine dyes.

The self-assembly of helical supramolecular structures from chiral building units is a basic principle of biological materials. The mesoscopic structure of a chiral molecular aggregate, which formed spontaneously from a nonchiral J-aggregating cyanine dye in aqueous solution, is presented. In single crystals (as shown in the picture) a coexistance of planar molecules with left- and right-handed twisted conformers of the same dye are found; the latter may act as templates to build up the helical superstructures.

The promotion of iron-induced generation of reactive oxygen species in nerve tissue by aluminum.

Aluminum is suspected to play a role in several neurological disorders. Reactive oxygen species (ROS) lead to oxidative stress, which is thought to be a possible mechanism for neurological damage. Interactions between aluminum and iron, a known promoter of prooxidant events, were studied in cerebral tissues using a fluorescent probe to measure rates of generation of ROS. Al2(SO4)3 alone failed to stimulate ROS production over a wide range of concentrations (50-1000 microM). The aluminum-deferrioxamine chelate in the absence of iron could also not potentiate ROS formation. However, Al2(SO4)3 potentiated FeSO4-induced ROS, with a maximal effect at 10 microM Fe and 500 microM Al. Kaolin, a hydrated aluminum silicate, did not potentiate iron-induced ROS formation. Ferritin had a minor stimulatory effect on ROS generation, but this was not potentiated by the concurrent presence of Al2(SO4)3. Transferrin had no effect on basal rates of ROS generation, but when Al2(SO4)3 was also present, ROS production was enhanced. It is concluded that: 1. There is a potentiation of iron-induced ROS by aluminum salts; 2. Free or complexed aluminum alone is not a key producer of ROS; and 3. High rates of ROS production are unlikely to be owing to the displacement by aluminum iron from its biologically sequestered locations.