Aggregation of organic dyes often
has consequences on their spectroscopic
properties in materials. Here, we study a new sterically hindered
boron-dipyrromethene (BODIPY), with adamantyl moieties grafted for
the first time on the BODIPY core. Its aggregation behavior was investigated
in poly(methyl methacrylate) (PMMA) and on drop-casted films by monitoring
absorption, fluorescence emission, relative quantum yield (ΦFluo,Rel), lifetime and time-resolved anisotropy. Aggregates
only appear from 0.067 mol·L–1. A multicomponent
analysis demonstrated that the aggregation process can be described
by three distinguishable components which correspond to a monomer
species (M) and J and H aggregates. The results also indicated a concentration
frontier: when the dye concentration increased up to 0.29 mol·L–1, the concentration of M decreased in favor of the
aggregates. ΦFluo,Rel is yet only divided by 5 compared
to the dye in solution. Above 0.29 mol·L–1,
an equilibrium between M and the J aggregates is established, showing
meanwhile a steady ΦFluo,Rel. The J aggregates are
found to be dimers, whereas the aggregation number is varying for
the H aggregates. Analysis of fluorescence and anisotropy decays showed
that the excitation energy was transferred from M to the J dimers,
and very probably trapped by H aggregates.
The polarization states of lasers are crucial issues both for practical applications and fundamental research. In general, they depend in a combined manner on the properties of the gain material and on the structure of the electromagnetic modes. In this paper, we address this issue in the case of solid-state organic lasers, a technology which enables to vary independently gain and mode properties. Different kinds of resonators are investigated: in-plane micro-resonators with FabryPerot, square, pentagon, stadium, disk, and kite shapes, and external vertical resonators. The degree of polarization P is measured in each case. It is shown that although TE modes prevail generally (P >0), kite-shaped micro-laser generates negative values for P , i.e. a flip of the dominant polarization which becomes mostly TM polarized. In general, we demonstrate that both the pump polarization and the resonator geometry can be used to tailor the polarization of organic lasers. With this aim in view, we, at last, investigate two other degrees of freedom, namely upon using resonant energy transfer (RET) and upon pumping the laser dye to a higher excited state. We then demonstrate that significantly lower P factors can be obtained.
BODIPYrrole: A general strategy for the design of novel BODIPY fluorophores based on pyrroles with polycondensed aromatic and metallocene substituents has been developed. The strategy involves the acylation of the condensed substituent and treatment of the acylated derivative (as oxime) with acetylene in MOH/DMSO (M = alkali metal) to give pyrroles that were then used for assembly of the BODIPY fluorophores (see scheme).
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