Abstract
The electrochemistry of homoleptic substituted phthalocyaninato rare earth double‐decker complexes M(TBPc)~2~ and M(OOPc)~2~ [M = Y, La...Lu except Pm; H~2~TBPc = 3(4),12(13),21(22),30(31)‐tetra‐tert‐butylphthalocyanine, H~2~OOPc = 3,4,12,13,21,22,30,31‐octakis(octyloxy)phthalocyanine] has been comparatively studied by cyclic voltammetry (CV) and differential pulse voltammetry (DPV) in CH~2~Cl~2~ containing 0.1 M tetra‐n‐butylammonium perchlorate (TBAP). Two quasi‐reversible one‐electron oxidations and three or four quasi‐reversible one‐electron reductions have been revealed for these neutral double‐deckers of two series of substituted complexes, respectively. For comparison, unsubstituted bis(phthalocyaninato) rare earth analogues M(Pc)~2~ (M = Y, La...Lu except Pm; H~2~Pc = phthalocyanine) have also been electrochemically investigated. Two quasi‐reversible one‐electron oxidations and up to five quasi‐reversible one‐electron reductions have been revealed for these neutral double‐decker compounds. The three bis(phthalocyaninato)cerium compounds display one cerium‐centered redox wave between the first ligand‐based oxidation and reduction. The half‐wave potentials of the first and second oxidations and first reduction for double‐deckers of the tervalent rare earths depend on the size of the metal center. The difference between the redox potentials of the second and third reductions for M^III^(Pc)~2~, which represents the potential difference between the first oxidation and first reduction of [M^III^(Pc)~2~]^−^, lies in the range 1.08−1.37 V and also gradually diminishes along with the lanthanide contraction, indicating enhanced π−π interactions in the double‐deckers connected by the smaller, lanthanides. This corresponds well with the red‐shift of the lowest energy band observed in the electronic absorption spectra of reduced double‐decker [M^III^(Pc′)~2~]^−^ (Pc′ = Pc, TBPc, OOPc). (© Wiley‐VCH Verlag GmbH & Co. KGaA, 69451 Weinheim, Germany, 2004)