Synthesis, Photophysical and Electronic Properties of a D‐π‐A Julolidine‐Like Pyrenyl‐o‐Carborane

Author:

Krebs Johannes1ORCID,Brändler Lisa1,Krummenacher Ivo1ORCID,Friedrich Alexandra1ORCID,Braunschweig Holger1ORCID,Finze Maik1ORCID,Curchod Basile F. E.2ORCID,Marder Todd B.1ORCID

Affiliation:

1. Institute for Inorganic Chemistry and Institute for Sustainable Chemistry & Catalysis with Boron Julius-Maximilians-Universität Würzburg Am Hubland 97074 Würzburg Germany

2. Centre for Computational Chemistry, School of Chemistry, Cantock's Close University of Bristol Bristol BS8 1TS United Kingdom

Abstract

AbstractWe synthesized 2‐(1‐1,2‐dicarbadodecaboranyl(12))‐6,6,12,12‐tetramethyl‐7,8,11,12‐tetrahydro‐6H,10H‐phenaleno[1,9‐fg]pyrido[3,2,1‐ij]quinoline (4), a julolidine‐like pyrenyl‐o‐carborane, with pyrene substituted at the 2,7‐positions on the HOMO/LUMO nodal plane. Using solid state molecular structures, photophysical data, cyclic voltammetry, DFT and LR‐TDDFT calculations, we compare o‐carborane and B(Mes)2 (Mes=2,4,6‐Me3C6H2) as acceptor groups. Whereas the π‐acceptor strength of B(Mes)2 is sufficient to drop the pyrene LUMO+1 below the LUMO, the carborane does not do this. We confirm the π‐donor strength of the julolidine‐like moiety, however, which raises the pyrene HOMO‐1 above the HOMO. In contrast to the analogous pyrene‐2‐yl‐o‐carborane, 2‐(1‐1,2‐dicarbadodecaboranyl(12))‐pyrene VI, which exhibits dual fluorescence, because the rate of internal conversion between locally‐excited (LE) and charge transfer (CT) (from the pyrene to the carborane) states is faster than the radiative decay rate, leading to a thermodynamic equilibrium between the 2 states, 4 shows only single fluorescence, as the CT state involving the carborane as the acceptor moiety in not kinetically accessible, so a more localized CT emission involving the julolidine‐like pyrene moiety is observed.

Funder

Julius-Maximilians-Universität Würzburg

Engineering and Physical Sciences Research Council

Publisher

Wiley

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