Hu Lei (584278)Shawkat M. Aly (1612759)Paul-Ludovic Karsenti (1406407)Daniel Fortin (327951)Pierre D. Harvey (1406404)
Azophenine,\n(α-C<sub>6</sub>H<sub>5</sub>NH)<sub>2</sub>(C<sub>6</sub>H<sub>5</sub>–NC<sub>6</sub>H<sub>2</sub>N–C<sub>6</sub>H<sub>5</sub>), well known to be non-emissive, was rigidified\nby replacing two amine protons by two difluoroboranes (BF<sub>2</sub><sup>+</sup>) and further functionalized at the <i>para</i>-positions of the phenyl groups by luminescent <i>trans</i>-ArCC–Pt(PR<sub>3</sub>)<sub>2</sub>-CC (<b>[Pt]</b>) arms [Ar = C<sub>6</sub>H<sub>4</sub> (R = Et), hexa(<i>n</i>-hexyl)truxene) (<b>Tru</b>; R = Bu)]. Two effects\nare reported. First, the linking of these <b>[Pt]</b> arms with\nthe central azophenine (C<sub>6</sub>H<sub>4</sub>–NC<sub>6</sub>H<sub>2</sub>(NH)<sub>2</sub>N–C<sub>6</sub>H<sub>4</sub>; <b>Q</b>) generates very low energy charge-transfer\n(CT) singlet and triplet excited states (<sup>3,1</sup>(<b>[Pt]</b>-to-<b>Q</b>)*) with absorption bands extending all the way\nto 800 nm. Second, the rigidification of azophenine by the incorporation\nof BF<sub>2</sub><sup>+</sup> units renders the low-lying CT singlet\nstate clearly emissive at 298 and 77 K in the near-IR region. DFT\ncomputations place the triplet emission in the 1200–1400 nm\nrange, but no phosphorescence was detected. The photophysical properties\nare investigated, and circumstantial evidence for slow triplet energy\ntransfers, <sup>3</sup><b>Tru</b>* → <b>Q</b>,\nis provided.
James A. W. ShoemakerJ. Stephen Hartman
Essam MetwallyAlaaeldine Sh. SalehH. A. El‐Naggar
Masaaki KatayamaYoshitaka MasudaToshikazu TarutaniSeizo Misumi
Dianne J. Luning Prak (1293090)Brian H. Morrow (2030230)Sabina Maskey (1922629)Judith A. Harrison (5937683)Jim S. Cowart (1293075)Paul C. Trulove (1293081)
Jhenny F. Galan (1777465)Edward Germany (1777471)Amanda Pawlowski (1777468)Lynette Strickland (1777462)Mary GraceI. Galinato (1777474)