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Homoatomic Sulfur Cations 141 Fig. 3 Optimized geometries and relative energies of all true S42+ minima at the B3PW91 level of theory [21] 5.2.2 S42+ Isomers Due to the high local D4h symmetry it appeared simple to obtain reliable quantum chemical results not only on the structure but also on the energet- ics of the S42+ dication. It was shown, however, that especially the calculation of S42+ required great care and the highest level of theory available in order to obtain reliable results (see thermodynamics section) [20]. From this pub- lication also followed that the only affordable and comparably fast computa- tional technique for the correct structural and energetic description of sulfur homopolyatomic cations is the hybrid HF-DFT level B3PW91 and its newer modified version MPW1PW91. In the following, therefore, the potential en- ergy surface of the gaseous S42+ dication was examined with the B3PW91 method and this investigation revealed the presence of at least five local minima (Fig. 3) [21]. From Fig. 3 it is clear that, as in the solid state, square planar S42+ (A) is the global minimum of all assessed isomers. It should be noted though that the second favorable isomer B has an unexpected non-classical highly p and p*-p* bonded structure and only the next all s bonded isomer C with a high relative energy of +155 kJ mol1 has a classically expected geometry with the tricoordinate sulfur atoms formally bearing the positive charge. 5.2.3 Exo-Endo S82+ MP2, B3LYP, BLYP, BP86, and HF levels were unsuccessfully [22] employed to optimize the geometry of isolated S82+ dication. By contrast, the B3PW91 and MPW1PW91 levels for the first time led to a geometry of gaseous S82+ similar to solid S82+ in S8(AsF6)2 including the three long transannular con-PDF Image | Topics in Current Chemistry
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