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New organomercury(II) compounds containing intramolecular N <f>→</f> Hg interactions: crystal and molecular structure of [2-(Me2NCH2)C6H4]HgCl and [2-(Me2NCH2)C6H4]Hg[S(S)PPh2]

Authors :
Bumbu, Oana
Silvestru, Cristian
Concepción Gimeno, M.
Laguna, Antonio
Source :
Journal of Organometallic Chemistry. Apr2004, Vol. 689 Issue 7, p1172. 8p.
Publication Year :
2004

Abstract

[2-(Me2NCH2)C6H4]HgCl (1) was prepared by reacting HgCl2 with [2-(Me2NCH2)C6H4]Li in diethyl ether. The reactions of 1 with the sodium or ammonium salt of the appropriate thiophosphinato ligand, in 1:1 molar ratio, afford the isolation of [2-(Me2NCH2)C6H4]Hg[S(S)PR2] [R=Me (2), Et (3), Ph (4)], [2-(Me2NCH2)C6H4]Hg[S(O)PPh2] (5) and [2-(Me2NCH2)C6H4]Hg[S(S)P(OiPr)2] (6). The compounds were investigated by IR and multinuclear NMR (1H, 13C and 31P) spectroscopy. The molecular structures of 1 and 4 were determined by single-crystal X-ray diffraction. Due to the strong intramolecular coordination of the N atom of the pendant CH2NMe2 arm [Hg(1)–N(1) 2.764(6) and 2.725(4) A˚ in 1 and 4, respectively] both compounds exhibit a T-shaped (C,N)HgX core in the molecular unit, with almost linear arrangement of the covalent bonds [C(1)–Hg(1)–Cl(1) 176.93(18)&#176; in 1, and C(1)–Hg(1)–S(1) 169.54(16)&#176; in 4]. The crystals of 1 contain discrete monomeric molecules, while the crystals of 4 contain dimer associations built through asymmetric bridging dithiophosphinato ligands [Hg(1)–S(1) 2.3911(16) A˚, Hg(1)&lt;f&gt;⋯&lt;/f&gt;S(2a) 3.102(2) A˚], thus resulting in an overall pseudo-trigonal bipyramidal (or seesaw) (C,N)HgS2 core, with the nitrogen atom and the weekly bonded sulfur atom in equatorial positions [N(1)–Hg(1)&lt;f&gt;⋯&lt;/f&gt;S(2a) 82.01(10)&#176;]. [Copyright &amp;y&amp; Elsevier]

Details

Language :
English
ISSN :
0022328X
Volume :
689
Issue :
7
Database :
Academic Search Index
Journal :
Journal of Organometallic Chemistry
Publication Type :
Academic Journal
Accession number :
12501956
Full Text :
https://doi.org/10.1016/j.jorganchem.2003.10.044