Pressure-induced intermetallic valence transition in BiNiO3

The valence state change of BiNiO3 perovskite under pressure has been investigated by a powder neutron diffraction study and electronic-state calculations. At ambient pressure, BiNiO3 has the unusual charge distribution Bi(3+)(0.5)Bi(5+)(0.5)Ni(2+)O3 with ordering of Bi(3+) and Bi(5+)charges on the A sites of a highly distorted perovskite structure. High-pressure neutron diffraction measurements and bond valence sum calculations show that the pressure-induced melting of the charge disproportionated state leads to a simultaneous charge transfer from Ni to Bi, so that the high-pressure phase is metallic Bi(3+)Ni(3+)O3. This unprecedented charge transfer between A and B site cations coupled to electronic instabilities at both sites leads to a variety of ground states, and it is predicted that a Ni-charge disproportionated state should also be observable.     

Supramolecular organization of light-harvesting porphyrin macrorings

Porphyrin‐based supramolecular nanostructures have been produced by the self‐assembly of porphyrin macrorings with three benzoic acid groups (Acid‐R) on each side of the rings through cooperative carboxyl–carboxyl hydrogen bonds. Structures of the organized Acid‐R were analyzed by AFM, and two clear distribution peaks were observed at 3 and 27 nm in the height‐distribution histogram. From the overall assessment, the higher objects are considered to be one‐dimensional structures standing vertically on the mica substrate. The height corresponds to an 11‐mer of a unit Acid‐R. Light‐harvesting functions were examined by using fluorescence titration, whereby an energy‐acceptor molecule (Tripod 2 ) was employed that strongly interacted with Acid‐R units (association constant: 2.0×10⁸ M ^?1), specifically from the inner pore. The titration results showed that the apparent stoichiometry [Tripod 2 ]/[Acid‐R] was <0.5, and that the value was concentration dependent. Titration results reasonably account for the scheme in which Tripod 2 only interacts with each terminal in the organized Acid‐R. The number of organization was fitted to a 10‐mer of Acid‐R in a 6.8×10^?7 M solution, and was consistent with that estimated from the AFM results. In the composites of organized Acid‐R/Tripod 2 , a singlet excitation energy transfer occurred among the Acid‐R units, and to Tripod 2 . The energy‐transfer rate constants were estimated by using the decamer model, which employed kinetic parameters obtained from steady‐state and time‐resolved fluorescence experiments.