NBN- and BNB-Phenalenyls: the Yin and Yang of Heteroatom-doped π Systems.
Alexander S ScholzJulian G MassothLennart StoessMichael BolteMarkus BraunHans-Wolfram LernerJan-Michael MewesMatthias WagnerThomas FroitzheimPublished in: Chemistry (Weinheim an der Bergstrasse, Germany) (2024)
NBN- and BNB-doped phenalenyls are isoelectronic to phenalenyl anions and cations, respectively. They represent a pair of complementary molecules that have essentially identical structures but opposite properties as electron donors and acceptors. The NBN-phenalenyls 1-4 considered here were prepared from N,N'-dimethyl-1,8-diaminonaphthalene and readily available boron-containing building blocks (i. e., BH 3 ⋅SMe 2 (1), p-CF 3 -C 6 H 4 B(OH) 2 (2), C 6 H 5 B(OH) 2 (3), or MesBCl 2 /iPr 2 NEt (4)). Treatment of 1 with 4-Me 2 N-2,6-Me 2 -C 6 H 2 Li gave the corresponding NBN derivative 5. The BNB-phenalenyl 6 was synthesized from 1,8-naphthalenediyl-bridged diborane(6), PhNH 2 , and MesMgBr. A computational study reveals that the photoemission of 1, 4, and 5 originates from locally excited (LE) states at the NBN-phenalenyl fragments, while that of 2 is dominated by charge transfer (CT) from the NBN-phenalenyl to the p-CF 3 -C 6 H 4 fragment. Depending on the dihedral angle θ between its Ph and NBN planes, compound 3 emits mainly from a less polar LE (θ >55°) or more polar CT state (θ <55°). In turn, the energetic preference for either state is governed by the polarity of the solvent used. An equimolar aggregate of the NBN- and BNB-phenalenyls 3 and 6 (in THF/H 2 O) shows a distinct red-shifted emission compared to that of the individual components, which originates from an intermolecular CT state.