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Dynamics and counterion-dependence of the structures of weakly bound Ag+-P4S3 complexes
Authors:Raabe Ines  Antonijevic Sasa  Krossing Ingo
Institution:1. Albert‐Ludwigs‐Universit?t Freiburg, Institut für Anorganische und Analytische Chemie, Albertstrasse 21, 79104 Freiburg i. Br., Germany, Fax: (+49)?761‐203‐6001;2. Ecole Polytechnique Fédérale de Lausanne, Institut des Sciences et Ingénierie Chimiques, Batochimie, 1015 Lausanne, Switzerland, Fax : (+41)?21‐693‐9355
Abstract:In an earlier publication (J. Am. Chem. Soc. 2002 , 124, 7111) we showed that polymeric cationic Ag(P4S3)n]+ complexes (n=1, 2) are accessible if partnered with a suitable weakly coordinating counterion of the type Al(ORF)4]? (ORF: poly‐ or perfluorinated alkoxide). The present work addresses the following questions that could not be answered in the initial report: How many P4S3 cages can be bound to a Ag+ ion? Why are these complexes completely dynamic in solution in the 31P NMR experiments? Can these dynamics be frozen out in a low‐temperature 31P MAS NMR experiment? What are the principal binding sites of the P4S3 cage towards the Ag+ ion? What are likely other isomers on the Ag(P4S3)n]+ potential energy surface? Counterion influence: Reactions of P4S3 with AgAl{OC(CH3)(CF3)2}4] (Aghftb]) and Ag{(CF3)3CO}3Al‐F‐Al{OC(CF3)3)}3] (Agal‐f‐al]) gave (P4S3)Aghftb]] ( 7 ) as a molecular species, whereas Ag2(P4S3)6]2+al‐f‐al]?2 ( 8 ) is an isolated 2:1 salt. We suggest that a maximum of three P4S3 cages may be bound on average to an Ag+ ion. Only isolated dimeric dications are formed with the largest cation, but polymeric species are obtained with all other smaller aluminates. Thermodynamic Born–Haber cycles, DFT calculations, as well as solution NMR and ESI mass spectrometry indicate that 8 exhibits an equilibrium between the dication Ag2(P4S3)6]2+ (in the solid state) and two Ag(P4S3)3]+ monocations (in the gas phase and in solution). Dynamics: 31P MAS NMR spectroscopy showed these solid adducts to be highly dynamic, to an extent that the 2JP,P coupling within the cages could be resolved (J‐res experiment). This is supported by DFT calculations, which show that the extended PES of Ag(P4S3)n]+ (n=1–3) and Ag2(P4S3)2]+ is very flat. The structures of α‐ and γ‐P4S3 were redetermined. Their variable‐temperature 31P MAS NMR spectra are discussed jointly with those of all four currently known Ag(P4S3)n]+ adducts with n=1, 2, and 3.
Keywords:NMR spectroscopy  phosphorus  silver  sulfur  weakly coordinating anions
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