Andreas Decken (1590190)Scott Greer (1877281)Friedrich Grein (1877284)Aaron Mailman (1486045)Birgit Mueller (1877272)Tressia A. P. Paulose (2821545)Jack Passmore (1877278)J. Mikko Rautiainen (1518712)Stephanie A. Richardson (2821547)Melbourne J. Schriver (1877287)Thomas K. Whidden (2821543)
One mole equivalent\nof gaseous SO<sub>2</sub> is absorbed by purple TDAE[O<sub>2</sub>SSO<sub>2</sub>](s), producing red, essentially spectroscopically\npure TDAE[O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>](s); under\nprolonged evacuation, the product loses SO<sub>2</sub>(g), regenerating\nTDAE[O<sub>2</sub>SSO<sub>2</sub>](s). Similarly, [NR<sub>4</sub>]<sub>2</sub>[O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>](s) (R = Et,\nMe) can be prepared, albeit at lower purity, from the corresponding\ntetraalkylammonium dithionites (prepared by a modification of the\nknown [NEt<sub>4</sub>]<sub>2</sub>[O<sub>2</sub>SSO<sub>2</sub>](s)\npreparation). While the [NEt<sub>4</sub>]<sup>+</sup> salt is stable\nat rt; the [NMe<sub>4</sub>]<sup>+</sup> salt has only limited stability\nat −78 °C. Vibrational spectra assignments for the anion\nin these salts were distinctly different from those for the anion\nin salts containing the long-known [O<sub>3</sub>SSSO<sub>3</sub>]<sup>2–</sup> dianion, the most thermodynamically stable form of\n[S<sub>3</sub>O<sub>6</sub>]<sup>2–</sup> (we prepared TDAE[O<sub>3</sub>SSSO<sub>3</sub>]·H<sub>2</sub>O(s) and obtained its\nstructure by X-ray diffraction and vibrational analyses). The best\nfit between the calculated ((B3PW91/6-311+G(3df) and PBE0/6-311G(d))\nand experimental vibrational spectra were obtained with the dianion\nhaving the [O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>]<sup>2–</sup> structure. Vibrational analyses of the three [O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>]<sup>2–</sup> salts prepared in this\nwork showed that the corresponding [O<sub>3</sub>SSO<sub>2</sub>]<sup>2–</sup> salts were present as a ubiquitous decomposition\nproduct. The formation of these new [O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>]<sup>2–</sup> dianion salts was predicted to\nbe favorable for [NMe<sub>4</sub>]<sup>+</sup> and larger cations\nusing a combination of theoretical calculations (B3PW91/6-311+G(3df))\nand volume based thermodynamics (VBT). Similar methods accounted for\nthe greater stabilities of the TDAE<sup>2+</sup> and [NEt<sub>4</sub>]<sup>+</sup> salts of [O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>]<sup>2–</sup> compared to [NMe<sub>4</sub>]<sub>2</sub>[O<sub>2</sub>SS(O)<sub>2</sub>SO<sub>2</sub>](s) toward irreversible decomposition\nto the corresponding [O<sub>3</sub>SSO<sub>2</sub>]<sup>2–</sup> salts. These salts represent the first known examples of a new class\nof poly(sulfur dioxide) dianion, [SO<sub>2</sub>]<sub><i>n</i></sub><sup>2–</sup> in which <i>n</i> > 2.
Junghwan Do (2102317)Ranko P. Bontchev (2425492)Allan J. Jacobson (1644922)
Jeongho Yeon (1406326)Sang-Hwan Kim (527119)Sau Doan Nguyen (1985821)Hana Lee (445860)P. Shiv Halasyamani (1261704)
Philip M. Almond (2509114)Thomas E. Albrecht-Schmitt (1370601)
Hai Tao XiaYu Fen LiuDe Fu Rong