Open Access Article
Satoru
Tsukada
a,
Nathan J.
O'Brien
a,
Naokazu
Kano
*a,
Takayuki
Kawashima
*a,
Jing-Dong
Guo
b and
Shigeru
Nagase
b
aDepartment of Chemistry, Graduate School of Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan. E-mail: kano@chem.s.u-tokyo.ac.jp; takayuki@chem.s.u-tokyo.ac.jp
bFukui Institute for Fundamental Chemistry, Kyoto University, Takano-Nishihiraki-cho, Sakyo-ku, Kyoto 606-8103, Japan
First published on 11th November 2016
The first dianionic compound bearing a bond between two pentacoordinated tin atoms, a distannate, was synthesized in a stable form by using two sets of an electron-withdrawing C,O-bidentate ligand on each tin atom. The structure of the distannate was determined by NMR spectroscopy and X-ray crystallographic analysis. The Sn–Sn bond of the distannate was shown to be a single bond featuring high s-character. The 1J(Sn–Sn) coupling constant was larger than that of Sn(sp3)–Sn(sp3) bonds found in most hexaorganodistannanes. This bond feature was also supported by computational studies. The Sn–Sn bond was cleaved by treatment with hydrochloric acid, which shows a different reactivity to the homonuclear bonds of pentacoordinated disilicates and digermanates.
O→Sn coordination made the tin atoms pentacoordinated.36 However, there is no report of a dianionic species containing a bond between two pentacoordinated ate-type tin atoms, a distannate, as far as we know. A reason for this is simply not ascribed to the instability of the ate-type structure of each tin atom as several stable pentacoordinated ate-type tin compounds, which show a trigonal bipyramidal (TBP) structure around the tin atom, have been synthesized by taking advantage of electron-withdrawing bidentate ligands.7,37–40
We previously reported the synthesis of disilicate 5
41,42 and digermanate 6,43 which are dianionic species containing a bond between two pentacoordinated ate-type silicon and germanium atoms, respectively. A tin analogue of 5 and 6 could be a challenging synthetic target considering the much smaller bond energy of the Sn–Sn bond in comparison to the Si–Si and Ge–Ge bonds.41,43 Disilicate 5 and digermanate 6 were successfully stabilized by taking advantage of four sets of an electron-withdrawing bidentate ligand. It was also presumed that these ligands could overcome the difficulties of stabilization of a distannate. Herein we report the synthesis and crystal structure of pentacoordinated distannate 7 bearing two bidentate ligands, –C6H4–2-C(CF3)2O–,44 on each tin atom. We also investigated the properties of the tin–tin bond by using 119Sn NMR spectroscopy and density functional theory (DFT) calculations.
37 (0.86 g, 1.0 mmol) (dried at 182 °C under reduced pressure before use) in THF (2 mL) was added a THF solution of lithium naphthalenide (0.47 M, 2.6 mL, 1.2 mmol) at −78 °C under argon. The mixture was stirred for 3 hours, then warmed to room temperature and stirred for a further 14 hours. The reaction mixture was concentrated under reduced pressure and the resulting residue was washed with Et2O to give a grey solid. The solid was dissolved in THF, filtered through a bed of Celite® and concentrated under reduced pressure to give a colorless solid. The solid was recrystallized from THF/n-hexane to give the distannate 7 (0.40 g, 48%) as a colorless solid; m.p. 226–230 °C. 1H NMR (300 MHz, THF-d8) δ 1.05 (t, 3JHH = 7.4 Hz, 24H), 1.49 (sext, 3JHH = 7.4 Hz, 16H), 1.73–1.82 (m, 16H), 3.35–3.41 (m, 16H), 6.98 (dt, 3JHH = 7.5 Hz, JHSn = 1.0 Hz, 4H), 7.11 (dt, 3JHH = 7.2 Hz, JHSn = 1.0 Hz, 4H), 7.35 (d, 3JHH = 7.5 Hz, 4H), 8.14 (dt, 3JHH = 6.9 Hz, JHSn = 27 Hz, 4H). 13C{1H} NMR (75 MHz, THF-d8) δ 13.77 (s), 20.32 (s), 24.44 (s), 59.09 (s), 83.74 (sept, 2JCF = 27 Hz), 125.36 (s, JCSn = 79 Hz (satellite peaks)), 125.79 (q, 1JCF = 288 Hz), 126.39 (q, 1JCF = 289 Hz), 126.49 (s, JCSn = 83 Hz (satellite peaks)), 127.36 (s), 137.27 (s, JCSn = 46 Hz (satellite peaks)), 141.00 (s, 1JCSn = 50 Hz, 2JCSn = 14 Hz (satellite peaks)), 148.74 (s). 19F NMR (282 MHz, THF-d8) δ −77.15 (d, 4JFF = 7.1 Hz, 12F), −77.52 (d, 4JFF = 7.9 Hz, 12F). 119Sn NMR (112 MHz, THF-d8) δ −94.9 (JSnSn = 15
532 Hz). LRMS (ESI, negative) m/z 1448 [M − (n-Bu)4N]−. Anal. Calcd for C68H88F24N2O4Sn2·2H2O: C, 47.30; H, 5.30; N, 1.62. Found: C, 47.17; H, 5.45; N, 1.71.
41 and digermanate 6
43 were synthesized by the reductive coupling of tetracoordinated spiro-silane and germane with lithium, but the analogous spirostannane has not been reported due to the high electrophilicity of the tin atom. However, pentacoordinated fluorostannate 8, bearing two sets of the electron-withdrawing C,O-bidentate ligand, is known to react with nucleophiles and was used for the synthesis of stannates.37 It is expected that a single electron reduction of 8 would give lithium fluoride elimination and generate the corresponding tin radical anion. Dimerization of the radical anion would yield the distannate similarly to the formation of the previously reported disilicates 5
41 and digermanates 6.43 Actually, reductive coupling of tetrabutylammonium fluorostannate 8
37 with lithium naphthalenide in THF gave distannate 7 in 48% yield as a dihydrate (Scheme 1). Distannate 7 was characterized by multinuclear NMR spectroscopy, elemental analysis, and single-crystal X-ray diffraction analysis. The pentacoordinated fluorostannate 8 was used to generate the corresponding tin radical anion in this reaction.
The crystal structure of 7 was determined by single-crystal X-ray diffraction analysis (Fig. 1). The tin-containing moiety was found to be a dianion and was accompanied by two separated tetrabutylammonium ions. The dianion has two pentacoordinated tin atoms, which are bonded to each other, showing its identity as a distannate. Distannate 7 shows a trigonal bipyramidal geometry around each crystallographically equivalent tin atom with two oxygen atoms at the apical positions and another tin and two carbon atoms at the equatorial positions. In other words, the Sn–Sn bond forms an equatorial bond on each tin atom.
The Sn1–Sn1* bond length (2.7522(14) Å) is similar to that of Ph3Sn–SnPh3 (2.770(4) Å)45 and the sum of the covalent radii (2.78 Å)46 indicates single bond character. Moreover, among the pentacoordinated Sn–Sn bonded compounds, the Sn1–Sn1* bond length of 7 is between the values of neutral distannanes 1 bearing bridging carboxylato ligands (2.692(3)–2.721 Å)27–31 and distannanes 2, 3, and 4 bearing chelating amine or imine ligands (2.8014(13)–2.831 Å).32–35 The Sn–O1 and Sn–O2 apical bond lengths (2.166(9) and 2.162(9) Å) are longer than the sum of the Sn–O covalent radii (2.05 Å),46 which is in accordance with the apical bonds of pentacoordinated species having a tendency of being long. Nevertheless, the apical Sn–O bond lengths are slightly longer than those of the tetrabutylammonium fluorostannate bearing the same bidentate ligands (2.101(6) and 2.110(6) Å).37 The O1–Sn1–O2 angle (166.0(4)°) of 7 is considerably narrower than that of fluorostannate 8 (178.7(3)°). The Sn1–O1 and Sn1*–O2* bonds are staggered relative to each other, as exhibited by the O1–Sn1–Sn1*–O2* torsion angle (58.6(4)°), to avoid the steric repulsion of the bulky bidentate ligands. The torsion angle of 7 is smaller than the O–Si–Si–O and O–Ge–Ge–O torsion angles of disilicate 5 (66.64(5)°) and digermanate 6 (60.79(19)°), respectively.41,43 This reflects a decrease in steric repulsion between the bulky bidentate ligands on the group 14 element atoms due to the longer bond lengths between the two tin atoms.
To investigate the temperature dependence of the structure of 7, variable temperature 19F NMR measurements were carried out over a range of 30–65 °C in THF-d8 (Fig. S9†). There was no change in the spectra, indicating no pseudorotation around the Sn atom in the temperature range. In the 119Sn-NMR spectrum of 7 in THF-d8, one singlet was observed at δSn −94.9 ppm accompanied by satellite peaks due to the coupling between 119Sn and 117Sn nuclei. The 119Sn chemical shift of 7 is reasonable for an anionic pentacoordinated tin nucleus coordinated by electron-withdrawing ligands as it is similar to other pentacoordinated tin allyl ate complexes, e.g. (n-Et4N)+[(1,2-C6H4C(CF3)2O–)2Sn(CH2CHCH2)]− (δSn −105.0 ppm).38 The 119Sn–117Sn coupling constant (1J(Sn–Sn) = 15
532 Hz) of 7 is similar to those of neutral pentacoordinated distannanes, e.g. Ph4Sn2(OOCCH3)21 [1J(Sn–Sn) = 16
120 Hz],31 but is much larger than those of distannanes, such as Ph3Sn–SnPh3 (1J(Sn–Sn) = 4281 Hz) and (t-Bu)(i-Pr)2Sn–Sn(t-Bu)(i-Pr)2 (1J(Sn–Sn) = 764 Hz).47 The small coupling constant of (t-Bu)(i-Pr)2Sn–Sn(t-Bu)(i-Pr)2 is due to the bulky ligands on the tin atoms, which decreases the s-character of the Sn–Sn bond. Thus, the large coupling constant 1J(Sn–Sn) of 7 indicates high s-character of the Sn–Sn bond.
To investigate the molecular orbital and the bonding properties of the distannate, DFT calculations on the dianion were carried out using the Gaussian 09 program.48 Geometry optimization was performed with the dispersion-corrected B3PW91-D3BJ method49,50 by using the [4333111/433111/43] basis set augmented by two d polarization functions (d exponents 0.253 and 0.078)51 and diffusion function (sp exponent 0.0174) for Sn52 and the 6-31+G(d) basis set for other atoms. The natural bond orbital analysis was performed using the NBO program.53 The optimized structure of the dianion of 7 reproduced the dianion of the crystal structure (see the ESI†). The highest occupied molecular orbital (HOMO) was mainly contributed by the bonding σ orbital of the Sn–Sn bond and the lone pairs of the oxygen atoms (Fig. 2). The lowest unoccupied molecular orbital (LUMO) was contributed not by the σ* orbital of the Sn–Sn bond, but mainly by the π* orbitals of the benzene rings. These molecular orbital features are almost the same as 5 and 6.41,43 The Wiberg bond index54 of the Sn–Sn bond is 0.843, indicating that the Sn–Sn bond of distannate 7 is a single bond and corresponds to the crystallographic analysis. Additionally, the natural bond orbital analysis shows sp2.35 hybridization of the tin atoms that constitute the Sn–Sn bond of the distannate. The high s-character of the Sn–Sn bond is consistent with the larger 1J(Sn–Sn) coupling constant of the distannate than that of the Sn(sp3)–Sn(sp3) bonds in most distannanes. Charge distributions of the dianion of 7 were estimated by the natural population analysis. The tin atoms are positively charged (qSn, +1.581), while the oxygen and carbon atoms bound to the tin atoms are negatively charged (qO, −0.865, qC, −0.430). The localization of the negative charges on the bidentate ligands avoids the electrostatic repulsion between the two anionic halves of the distannate. The quantity of positive charge on the tin atoms was found to be larger than those of the silicon 5 (qSi, +1.393)41 and the germanium 6 (qGe, +1.30)43 atoms. This is a result of the high polarizability of the tin atom in comparison to the silicon and the germanium atoms.
Mass spectroscopic analysis showed an ion peak of m/z 1448, assigned to the dianion part with a tetrabutylammonium ion of distannate 7, indicating its stability in the gas phase. Distannate 7 was also stable to air and moisture and could be handled without precautions. However, the reaction of 7 with 20 equivalents of 1 M aqueous hydrochloric acid caused its degradation. Analysis of the 1H and 19F NMR spectra (Fig. S10 and S11†) of the reaction mixture shows the formation of an intermediate, thought to be the mono- or diprotonated distannate. This intermediate was shown to have a 119Sn NMR chemical shift at δSn −88.6 ppm (Fig. S12†), which is different from the literature value of chlorostannate (δSn −127.6 ppm).37 Further reaction of this intermediate cleaved the Sn–Sn bond and gave clean conversion to chlorostannate 9 (Scheme 2). The reactivity of 7 is different from that of 5 and 6, both of which underwent protonation on oxygen atoms bonded to silicon and germanium atoms without homonuclear bond cleavage, upon treatment with hydrochloric acid.41–43 This result shows that the Sn–Sn bond of the distannate is weaker than the Si–Si and Ge–Ge bonds of the disilicate and digermanate, respectively, under the same conditions.
Footnote |
| † Electronic supplementary information (ESI) available: NMR spectral charts of 7 and 9, summary of the optimized structures, and Cartesian coordinates of the dianion part of 7. CCDC 1501994. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c6dt03503e |
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