Abstract
Truxenone (Tr) with high C3h symmetry forms crystalline radical anion and dianion salts. The {Bu3MeP+}(Tr·−)(1) and {Cp*2Co+)}(Tr·‐).2C6H4Cl2(2) show intense low‐energy absorption up to 2000nm. Calculations predict Jahn–Teller distortions for Tr·‐, which are enhanced by the asymmetric approach of cations to Tr·‐, leading to C=O bond length alternation and EPR signal asymmetry in 2. Two cesium ions form short contacts of 3.07–3.35Å with oxygen atoms of Tr2‐ in {Cryptand[2.2.2](Cs+)}2(Tr2‐)(3), linking the dianions into a 1D polymer. Calculations suggest a triplet state for the dianions, but the unsymmetric approach of Cs+ to the oxygen atoms of Tr2‐ stabilizes the singlet ground state. The triplet state is populated above 100K. An estimated singlet–triplet energy gap is 344±7K. Radical anions of Tr·‐ coordinate with one d‐ or f‐metal, forming {Cp*2Co+}{TbIII(TMHD)3×Tr}‐.1.5C7H8(4) and {Cp*2Co+}{MnII(acac)2×Tr}‐.2.4C6H4Cl2(5). Strong antiferromagnetic TbIII–Tr·‐ coupling (J =−7.6cm−1) aligns spins of TbIII and Tr·‐ antiparallel in 4. The χMT value of 3.32 emu×K/mol at 300K for 5 with high‐spin MnII is lower‐than‐expected. That indicates a spin state of S=2 owing to the antiparallel alignment of MnII and Tr·‐ spins. Strong MnII–Tr·‐ coupling arising from the spin density localization on the oxygen coordinated to MnII. Complexes with metals demonstrate low‐energy absorption with maxima at 1504–1740nm.
Published Version
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