Gilles Ulrich

The chemistry of Bodipy: A new El Dorado for fluorescence tools

In the steadily expanding field of fluorescent dyes, labels and electroluminescent materials difluoroboron-dipyrromethenes play a prominent role. The review highlights recent advances made with these boron-stabilized cyanine dyes. The chemistry at the boron atom and increase of delocalization on the organic core allows one to address the problems of Stokes’ shifts, colours and emission wavelengths spanning from green to the NIR. The outcome is a diversity of molecules prepared by different strategies and exhibiting interesting and tunable spectroscopic, electrochemical and chemical properties. This perspective article describes the scope and spectroscopic attributes of this new class of fluorescent dyes amenable to applications in various disciplines.

Luminescent Materials: Locking π-Conjugated and Heterocyclic Ligands with Boron(III)

Multidisciplinary research on novel organic luminescent dyes is propelled by potential applications in plastic electronics and biomedical sciences. The construction of sophisticated fluorescent dyes around a tetrahedral boron(III) center is a particular approach that has fueled the creativity of chemists. Success in this enterprise has been readily achieved with simple synthetic protocols, the products of which display unusual spectroscopic behavior. This account is a critical review of recent advances in the field of boron(III) complexes (excluding BODIPYs and acetylacetonate boron complexes) involving species displaying similar coordination features, and we outline their potential development in several disciplines.

Color Tuning in New Metal‐Free Organic Sensitizers (Bodipys) for Dye‐Sensitized Solar Cells

Fun in the sun! A strategy has been devised for functionalizing and solubilizing boron dipyrromethene (Bodipy) dyes at the central boron atom and changing the color by increasing delocalization on the central core. This approach leads to the formation of stable B-C[triple bond]C and pyrrole--C=C linkages suitable for use in TiO(2)-sensitized devices (see figure).

Multi-donor molecular bulk heterojunction solar cells: improving conversion efficiency by synergistic dye combinations

Molecular bulk heterojunction solar cells with a power conversion efficiency of 1.70% have been fabricated using as donor BODIPY dyes with complementary light-harvesting properties.

Water-Soluble BODIPY Derivatives

New, water-soluble BODIPY dyes have been readily obtained from various BODIPY cores by reactions involving the introduction of novel sulfonated peptide chains by either coupling or substitution to give dimethylpropargylamine derivatives subsequently quaternized by reaction with propanesultone.

Length Dependence for Intramolecular Energy Transfer in Three- and Four-Color Donor-Spacer-Acceptor Arrays

A series of donor-spacer-acceptor triads has been synthesized and fully characterized. Both donor and acceptor units are built from boron dipyrromethene (BODIPY) dyes but they differ in their respective conjugation lengths, and thereby offer quite disparate optical properties. The spacer units comprise an oligomer of 1,4-phenylene-diethynylene repeat units and allow the boron-boron separation distance to be varied progressively from 18 to 38 A. A notable feature of this series is that each subunit can be selectively excited with monochromatic light. Highly efficacious electronic energy transfer (EET) occurs from the first-excited singlet state localized on the conventional BODIPY dye to its counterpart resident on the expanded BODIPY-based nucleus, but the rate constant follows a nonlinear evolution with separation distance. Overall, the rate of EET falls by only a factor of 4-fold on moving from the shortest to the longest spacer. This shallow length dependence is a consequence of the energy gap between donor and spacer units becoming smaller as the molecular length increases. Interestingly, a simple relationship exists between the measured electronic resistance of the spacer unit and the Huang-Rhys factor determined by emission spectroscopy. Both parameters relate to the effective conjugation length. Direct illumination of the spacer unit leads to EET to both terminals, followed by EET from conventional BODIPY to the expanded version. In each case, EET to the expanded dye involves initial population of the second-singlet excited state, whereas transfer from spacer to the conventional BODIPY dye populates the S(2) state for shorter lengths but the S(1) state for the longer analogues. The rate of EET from spacer to conventional BODIPY dye, as measured for the corresponding molecular dyads, is extremely fast (>10(11) s(-1)) and scales with the spectral overlap integral. The relative partitioning of EET from the spacer to each terminal is somewhat sensitive to the molecular length, with the propensity to populate the conventional BODIPY dye changing from 65% for N = 0 to 45% for N = 2. The most likely explanation for this behavior can be traced to the disparate spectral overlap integrals for the two dyes. These systems have been complemented by a molecular tetrad in which pyrene residues replace the fluorine atoms present on the conventional BODIPY-based dye. Here, rapid EET occurs from pyrene to the BODIPY dye and is followed by slower, long-range EET to the opposite terminal. Such materials are seen as highly attractive solar concentrators when dispersed in transparent plastic media and used under conditions where both inter- and intramolecular EET operate.

An Artificial Light-Harvesting Array Constructed from Multiple Bodipy Dyes

An artificial light-harvesting array, comprising 21 discrete chromophores arranged in a rational manner, has been synthesized and characterized fully. The design strategy follows a convergent approach that leads to a molecular-scale funnel, having an effective chromophore concentration of 0.6 M condensed into ca. 55 nm(3), able to direct the excitation energy to a focal point. A cascade of electronic energy-transfer steps occurs from the rim to the focal point, with the rate slowing down as the exciton moves toward its ultimate target. Situated midway along each branch of the V-shaped array, two chromophoric relays differ only slightly in terms of their excitation energies, and this situation facilitates reverse energy transfer. Thus, the excitation energy becomes spread around the array, a situation reminiscent of a giant holding pattern for the photon that can sample many different chromophores before being trapped by the terminal acceptor. At high photon flux under conditions of relatively slow off-load to a device, such as a solar cell, electronic energy transfer encounters one or more barriers that hinder forward progress of the exciton and thereby delays arrival of the second photon. Preliminary studies have addressed the ability of the array to function as a sensitizer for amorphous silicon solar cells.

Facile Synthesis of Highly Fluorescent Boranil Complexes

Complexation of a large variety of Anils (aniline-imines) with boron(III) precursors provides stable Boranils, some of which have been structurally characterized. Analysis of their optical properties reveals that the fluorescence stems from an intraligand charge transfer (ILCT) state with the best quantum yields reaching 90%. Chemistry on the Boranils allows grafting of photoactive modules acting as energy antennae for borondipyrromethene (Bodipy) and subphtalocyanine (SubPc) fluorophores.

Solid‐State Gas Sensors Developed from Functional Difluoroboradiazaindacene Dyes

This article describes the synthesis and characterization of several new difluoroboradiazaindacene (BODIPY) dyes functionalized at the central 8-position by a phenyliodo, phenylheptynoate or phenylheptynoic fragment and at the 3- or 3/5-position(s) by 4-dimethylaminophenylstyryl residue(s). Single-crystal structural determinations confirm the planarity of the dyes, while the absorption and fluorescence spectroscopic properties are highly sensitive to the state of protonation (or alkylation) of the terminal anilino donor group(s). Reversible color tuning from green to blue for absorption and from colorless (i.e., near-IR region) to red for fluorescence is obtained on successive addition of acid and base. The difunctionalized derivative is especially interesting in this respect and shows two well-resolved pK(a) values of 5.10 and 3.04 in acetonitrile. Addition of the first proton causes only small spectral changes and deactivates the molecule towards addition of the second proton. It is this latter step that accommodates the large change in absorption and emission properties, due to the reversible extinction of the intramolecular charge-transfer character inherent to this type of dye. The main focus of the work is the covalent anchoring of the dyes to inert, porous polyacrylate beads so as to form a solid-state sensor suitable for analysis of gases or flowing liquids. The final material is highly stable--its performance is undiminished after more than one year--and fully reversible over many cycles. The sensitivity is such that reactions can be followed by the naked eye and the detection limit is about 600 ppb for HCl and about 80 ppb for ammonia. Trace amounts of diphosgene can be detected, as can alkylating agents. The sensing action is indiscriminate and also operates when the beads are dispersed in aqueous media.

Tailoring the Properties of Boron−Dipyrromethene Dyes with Acetylenic Functions at the 2,6,8 and 4-B Substitution Positions

Substitution of F-Bodipy with alkynylaryl residues at boron, at the pyrrolic core or at the meso position, provides unique tri-, tetra-, and pentasubstituted dyes. Substitution at the (pyrrolic) 2,6-positions provides substantial red shifts with quantum yields in the 40-90% range and excited-state lifetimes of 3-7 ns. ON/OFF fluorescence switching can be produced by protonation of dibutylamino subunits.