Stepwise neutral-ionic phase transitions in a covalently bonded donor/acceptor chain compound

Neutral (N)-ionic (I) transitions in organic donor (D)/acceptor (A) charge-transfer complexes are intriguing because a 'reservoir of functions' is available. For systematically controlling N-I transitions, tuning the ionization potential of D and the electron affinity of A is extremely important. However, the effect of Coulomb interactions, which likely causes a number of charge-gap states at once in a system bringing about stepwise transitions, is a long-standing mystery. Here, we show definite evidence for stepwise N-I transitions caused by contributions from anisotropic interchain Coulomb interactions in a metal-complex-based covalently bonded DA chain compound, [Ru(2)(2,3,5,6-F(4)PhCO(2))(4)(DMDCNQI)]·2(p-xylene) (1; 2,3,5,6-F(4)PhCO(2)(-) = 2,3,5,6-tetrafluorobenzoate; DMDCNQI = 2,5-dimethyl-N,N'-dicyanoquinonediimine), where the [Ru(2)(II,II)(2,3,5,6-F(4)PhCO(2))(4)] moiety has a paddlewheel diruthenium(II,II) motif with a Ru-Ru bond. An intermediate-temperature phase involving self-organized N and I chains was observed in the temperature range between 210 K (= T(2)) and 270 K (= T(1)) with N phase at T > T(1) and I phase at T < T(2). Accompanying the charge transitions, the spin-ground states as well as the ferrimagnetic ordering in the I phase vary. The stepwise feature of the N-I transition with a highly sensitive magnetic response should bring about new dynamical functionalities associated with charge, spin, and lattice.     

The proton uptake channel of bacteriorhodopsin as studied by a photoelectrochemical method

A series of the mutant proteins (D96N, D96N/D85N, D115N, L93T, T46V, V49A) where the residues are located at the cytoplasmic domain of bacteriorhodopsin (bR) were studied photoelectrochemically and their photocurrent response characteristics at the electrode/electrolyte interface were compared with those of the wild-type bR. While the wild-type bR of normal proton pumping activity yields symmetrical cathodic (positive) and anodic (negative) responses, corresponding to proton release and proton uptake, respectively, these mutants, with the exception of D115N, showed diminished amplitudes in the negative response. This indicates retardation of proton translocation from the cytoplasmic surface to the retinal Schiff base. The mutation that gave the strongest influence on the negative response was D96N while moderate influence was obtained with L93T, T46V, and V49A. These results suggest that residues other than D96 also participate in the cytoplasmic proton uptake channel, either by interacting with D96 directly or by forming a hydrogen-bonded network with water molecules. The D96N/D85N double mutant yielded little response at neutral pH, but the response was partially recovered by addition of azide, while it was fully recovered in the single mutant D96N. The D115N mutant showed the response profile that closely resembles the wild-type, indicating that D115 is not crucially involved in the event of proton transfer relay at the cytoplasmic region. It was also found that every mutant in this study releases protons prior to uptake at the other membrane surface, as does the wild-type.     

Reducible properties of draw temperature,rate of strain and filler content in tensile yield stress of polymethylmethacrylate filled with ultrafine particles

The yield stress of polymethylmethacrylate (PMMA) composites filled with ultrafine SiO₂ particles was measured as a function of the draw temperature, rate of strain and filler content. The yield stress of the composites increased with increasing filler content and decreasing filler size. The tensile yield stress was found to be reducible with regard to draw temperature, rate of strain and filler content. At a given filler content, a master curve was obtained for the yield stress plotted versus the logarithm of the strain rate. The Arrhenius plot of the shift factors (a _T ) used to produce the strain rate-temperature master curve formed a single curve for all sizes and loadings of the filler. The master curves obtained for different loadings of a filler of given size could be further reduced into a master-master curve by shifting them along the axis of strain rate, with the logarithm of the second shift factors (loga _c ) proportional to the 4/5th power of the filler volume fraction (V _f ). The proportionality constant and the exponent represent the extent of the filler reinforcing effect in the polymer. These values were found to be correlated with the critical surface tension of the polymers.     

Spin Ice-like Magnetic Relaxation of a Two-dimensional Network based on Manganese(III) Salen-type Single-Molecule Magnets

Spin ice is an exotic type of magnetism displayed by bulk rare-earth pyrochlore oxides. We discovered a spin ice-like magnetic relaxation of [{Mn(saltmen)}₄{Mn(CN)₆}](ClO₄)⋅13 H₂O (saltmen²⁻=N,N′-(1,1,2,2-tetramethylethylene)bis(salicylideneiminate)). This magnetic system can be considered as a two-dimensional network of Mn^III salen-type single-molecule magnets (SMMs) in which each SMM unit (S_T=4) has two orthogonally oriented axial anisotropies and is connected ferromagnetically through the [Mn(CN)₆]³⁻ unit (S=1). This work illustrates that a two-dimensional SMM network with competition between the ferromagnetic interaction and local noncollinear magnetic anisotropies on SMMs is a new type of magnetic system exhibiting slow relaxation of magnetization with a Davidson-Cole-type broad distribution of the relaxation time.     

The Effect of Pre-solvation in the Ground State on Photoinduced Electron Transfer in Ionic Liquids

Photoinduced intramolecular charge transfer (CT) dynamics of the asymmetric and symmetric molecules, 4-(9-anthryl)-N,N-dimethylaniline (ADMA) and 9,9′-bianthryl (BA), was investigated by means of time-resolved fluorescence (TRF) spectroscopy and compared with the solvation dynamics of coumarin 153 (C153) in several ionic liquids (ILs). The normalized dynamic Stokes shift (DSS) function for the CT state emission of ADMA in the sub-ns to ns time scale is almost the same as those of BA and C153 in most of the ILs studied, in spite of the much larger Stokes shift of ADMA compared to those of BA and C153. On the other hand, the contribution from ultrafast DSS within 30 ps, which was undetectable with the time resolution in the present study, was estimated to be smaller for BA than that for ADMA. Meanwhile, in phosphonium IL, the DSS in sub-ns to ns time range was solute dependent. This peculiarity in phosphonium IL is discussed from the viewpoint of the hierarchy of the solvation dynamics.     

Synthesis of Heterodinuclear Hemisalen Complexes on a Hexaarylbenzene Scaffold and their Application for the Cross‐Pinacol Coupling Reaction

Intermolecular cross‐pinacol coupling reaction between aliphatic and aromatic aldehydes by using heterodinuclear hemisalen complexes 1 _cis with vanadium(V) and titanium(IV) on a hexaarylbenzene scaffold is reported. Our ligand design is based on the individual activation of two aldehydes by vanadium and titanium, which are positioned with a suitable space on the rigid scaffold. Ligands such as 1 _cis were synthesized by Diels–Alder addition and decarbonylation reaction, followed by condensation of dialdehyde 3 _cis with various aminophenols. The influence of the substituents on the ligands on the pinacol coupling reaction was investigated. As a result, the reductive coupling reaction between aliphatic and aromatic aldehydes by using a catalytic amount of 1 _cis in the presence of Me₃SiCl and Zn provided the corresponding cross‐coupled 1,2‐diol in good yields with high cross‐selectivity.