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A Tale of Two Complexes, [PtMe n (RNCHCHNR)] ( n = 2 and n = 4, R = Cyclohexyl): Why do Pt II and Pt IV Complexes Exhibit Virtually Identical Redox Behavior and Colors?
Author(s) -
Hasenzahl Steffen,
Hausen HansDieter,
Kaim Wolfgang
Publication year - 1995
Publication title -
chemistry – a european journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.687
H-Index - 242
eISSN - 1521-3765
pISSN - 0947-6539
DOI - 10.1002/chem.19950010114
Subject(s) - chemistry , hyperfine structure , ligand (biochemistry) , crystallography , electron paramagnetic resonance , excited state , absorption spectroscopy , ground state , ion , metal , photochemistry , stereochemistry , nuclear magnetic resonance , atomic physics , physics , biochemistry , receptor , quantum mechanics , organic chemistry
In spite of their very similar cyclic voltammograms, absorption spectra, and solvatochromic behavior, the two 1,4‐diazabutadiene title complexes exhibit markedly different photoreactivities and underlying electronic structures, as evident from absorption and EPR spectra of the persistent anion radical forms. The lowest excited state of the nonphotoreactive Pt II system [(CyNCHCHNCy)‐PtMe 2 ] has MLCT (metal‐to‐ligand charge‐transfer, 5d → π*) character, and the EPR spectrum of the corresponding anion radical at 〈g〉 = 2.016 exhibits sizable metal/ligand orbital mixing. On the other hand, the structurally characterized Pt IV complex [(CyNCHCHNCy)‐PtMe 4 ] ( C 2/c; a = 2021.6(2), b = 805.3(1), c = 1254.2(1) pm; β = 111.05(1)°; V = 1905.7(4) × 10 6 pm 3 ; Z = 4) has a lowlying photoreactive LLCT (ligand‐to‐ligand charge‐transfer, σ PtC → π*) excited state in which the axial PtC bonds are activated, as already suggested by the longer PtC(ax) bonds (214.0(8) pm) relative to PtC(eq) in the ground state (204.5(5) pm). The anion radical of the Pt IV complex has lost the long‐wavelength absorption band in the visible; it shows a well‐resolved EPR spectrum at 〈g〉 = 1.9945 with π‐ligand and 195 Pt hyperfine structure and a small g anisotropy. A qualitative MO scheme is presented to account for the similar frontier‐orbital energy differences despite dissimilar underlying electronic structures.