Reduction of 2-(BMes2)pyrene (B1) and 2,7-bis(BMes2)pyrene (B2) gives rise to anions with extensive delocalization over the pyrenylene bridge and between the boron centers at the 2- and 2,7-positions, the typically unconjugated sites in the pyrene framework. One-electron reduction of B2 gives a radical anion with a centrosymmetric semiquinoidal structure, while two-electron reduction produces a quinoidal singlet dianion with biradicaloid character and a relatively large S0-T1 gap. These results have been confirmed by cyclic voltammetry, X-ray crystallography, DFT/CASSCF calculations, NMR, EPR, and UV-vis-NIR spectroscopy.
Interface
structures of a variety of molecular p-type semiconductors
in heterojunction with fullerene C60 were generated in
molecular dynamic simulations. Using the dimer method (i.e., dimers
were used as the quantum-mechanical system) along with a continuum
solvation approach and macroscopic electric fields, energetic profiles
of the interfaces of organic solar cells (OSCs) were calculated. Several
important loss mechanisms, such as exciton trapping, charge trapping,
and interfacial charge-transfer traps, were observed. Structure–property
relationships were established. They reveal that apart from the molecular
orientation and dipolarity, molecular size is an important parameter
that influences potential loss mechanisms.
We present an analysis of the optoelectronic properties of merocyanine dyes by means of VBSCF, TDDFT and high-level ab initio calculations. The electronic structure of merocyanines can be described as a superposition of two resonance structures, a neutral and zwitterionic one. Calculated VB weights for these resonance structures demonstrate the importance of strong accepting groups in increasing the weight of the zwitterionic structures of different merocyanines. The dependence of exciton and charge reorganization energies on the VB weights' composition is analyzed, demonstrating that the special case of equal contributions of both structures, the so-called cyanine limit, goes along with minimal exciton and charge reorganization energies. For the latter, it is shown that the external (outer-sphere) reorganization energy plays a crucial role. Furthermore, a careful investigation of the excited-state behavior of merocyanines indicates that a possible excited-state torsion might be another important parameter for merocyanine-based optoelectronic devices, while internal (innersphere) charge reorganization energies of a variety of merocyanines are in a typical range for molecular semiconductors.
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