Surface-initiated synthesis of poly(3-methylthiophene) from indium tin oxide and its electrochemical properties

Poly(3-methylthiophene) (P3MT) was synthesized directly from indium tin oxide (ITO) electrodes modified with a phosphonic acid initiator, using Kumada catalyst transfer polymerization (KCTP). This work represents the first time that polymer thickness has been controlled in a surface initiated KCTP reaction, highlighting the utility of KCTP in achieving controlled polymerizations. Polymer film thicknesses were regulated by the variation of the solution monomer concentration and ranged from 30 to 265 nm. Electrochemical oxidative doping of these films was used to manipulate their near surface composition and effective work function. Doped states of the P3MT film are maintained even after the sample is removed from solution and potential control confirming the robustness of the films. Such materials with controllable thicknesses and electronic properties have the potential to be useful as interlayer materials for organic electronic applications.     

The one‐electron oxidation product of a metallocenyl‐terminated cyanine

The 1‐(2,3,4,5,1′,2′,3′,4′‐octa­methyl­ferrocen‐1‐yl)‐3‐(ruth­eno­cen­yl)­allylium cation readily undergoes one‐electron oxidation to a dication in which an octa­methyl­ferrocenium moiety is bridged by a vinyl­ene group to a [(η⁶‐fulvene)(η⁵‐cyclo­penta­dienyl)­ruthenium]⁺ moiety. In the title compound, 1‐(2,3,4,5,1′,2′,3′,4′‐octa­methyl­ferrocen‐1‐yl)‐3‐(ruth­eno­cen­ylidene)prop‐1‐enium(2+) bis­(tetra­fluoro­borate), [Fe­Ru­(C₅H₅)(C₉H₁₃)(C₁₇H₁₉)]­(BF₄)₂, the C—C bond lengths in the bridge (average for two independent mol­ecules) are, starting from the ipso octa­methyl­ferrocenium carbon and ending at the exo carbon of the coordinated fulvene, 1.455 (6), 1.344 (3) and 1.449 (8) Å, indicating a localized electronic structure.     

Octafluoronaphthalene–diphenylacetylene (1/1)

The structure of the title complex, C₁₀F₈·C₁₄H₁₀, comprises mixed stacks of alternating di­phenyl­acetyl­ene and octa­fluoro­naphthalene mol­ecules, both lying at inversion centres and parallel to within 8.6 (1)°, in contrast with the herring‐bone packing observed in crystals of either pure component.     

Thermodynamic equilibrium between locally excited and charge-transfer states through thermally activated charge transfer in 1-(pyren-2′-yl)-o-carborane

Reversible conversion between excited-states plays an important role in many photophysical phenomena. Using 1-(pyren-2′-yl)-o-carborane as a model, we studied the photoinduced reversible charge-transfer (CT) process and the thermodynamic equilibrium between the locally-excited (LE) state and CT state, by combining steady state, time-resolved, and temperature-dependent fluorescence spectroscopy, fs- and ns-transient absorption, and DFT and LR-TDDFT calculations. Our results show that the energy gaps and energy barriers between the LE, CT, and a non-emissive ‘mixed’ state of 1-(pyren-2′-yl)-o-carborane are very small, and all three excited states are accessible at room temperature. The internal-conversion and reverse internal-conversion between LE and CT states are significantly faster than the radiative decay, and the two states have the same lifetimes and are in thermodynamic equilibrium.

Reversible conversion between excited-states is key to many photophysical phenomena. We studied the equilibrium between LE and CT states by time-resolved and temperature-dependent fluorescence, fs- and ns-transient absorption, and LR-TDDFT calculations.     

Solvent effects on the vibronic one-photon absorption profiles of dioxaborine heterocycles

The vibronic profiles of one-photon absorption spectra of dioxaborine heterocycles in gas phase and solution have been calculated at the Hartree-Fock and density-functional-theory levels. The polarizable continuum model has been applied to simulate the solvent effect, while the linear coupling model is used to compute the Franck-Condon and Herzberg-Teller contributions. It is found that a good agreement between theory and experiment can be achieved when the solvent effect and electron correlation are taken into account simultaneously. For the first excited charge-transfer state, the maximum of its Herzberg-Teller profile is blueshifted from that of the Franck-Condon profile. The shifted energy is found to be around 0.2 eV, which agrees well with the measured energy difference between two- and one-photon absorptions of the first excited state.