Christoph
Marschner
Institute of Inorganic Chemistry, Graz University of Technology, 8010 Graz, Austria
First published on 28th May 2025
The last few years have witnessed exciting development in the chemistry of silylated rare earths and heavier f-elements. First examples of silylated lanthanum (La) and praseodymium (Pr) complexes have been reported so that currently out of all lanthanides only for the radioactive promethium (Pm) silylated complexes are unknown. Previously unknown U(III) silyl complexes have also been described. Spectacular examples of the elusive trisilylated complexes of lanthanides and actinides have been presented. These show unusual magnetic properties, making them susceptible to facile 29Si NMR spectroscopic characterization, which could be rather difficult for compounds with diminished silylation degree. Novel silylene complexes were shown to catalyze hydrosilylation reactions. The novel compound class of silole coordinated f-element complexes was introduced by La and erbium (Er) complexes with the latter exhibiting single molecule magnetic properties.
An excellent and detailed compilation of the chemistry of silylated f-element compounds until 2020 was published recently by Réant, Liddle, and Mills.7 Following their summary, it is possible to come to a number of conclusions. For instance, at 2020, of the 15 lanthanides, there were no known examples for silylated complexes of La, Pr, and Pm and only one or two examples for Ce, Nd, Tb, Dy, Er, and Lu, each. At that time, the by far best studied element was Yb with 15 silylated examples followed by Sm with 11 examples and Eu and Tm with 5 examples, each. All reported silylated Eu and most of the Yb complexes featured the metal in the oxidation state +2. While most of the divalent complexes were disilylated, much less disilylated trivalent complexes had been prepared, left alone examples of trisilylated complexes. In 2020, the number of silylated actinide complexes amounted to 3 Th and 5 U complexes, all of them monosilylated.7 All of the uranium complexes featured U(IV).
A reason for the long-lasting neglect of silyl f-element chemistry may to be that many of these compounds are paramagnetic. Typically, strong paramagnetism causes problems with NMR spectroscopic characterization. Even if meaningful spectra can be obtained, their diagnostic value is often hard to assess. This is especially true for hetero-nuclei with diminished receptivity such as 29Si.
The present account attempts to provide an overview over the work on silylated rare earths and heavier f-elements, since the mentioned review by Réant, Liddle, and Mills.7
To address problems arising from ligand-dissociation induced decomposition, our research group has sought to suppress such processes by use of multidentate ligands such as oligosilanylene diides and dimethoxyethane (DME) as solvent. In addition, the attachment of additional Lewis basic sites to the ligand, which was successfully applied to trialkyl complexes such as Ln(CH2C6H4-o-NMe2)3,10 was attempted.8 Utilizing the 1,5-oligosilanylene diide 1 containing a disiloxane unit, it was possible to isolate first examples of silylated La and Pr complexes as well as a first example of a structurally characterized Si–Dy complex along with complexes of Y, Ce, Sm, Tb, and Er (2M) (Scheme 1).11
Although a fair number of silylated rare earths and f-element complexes have been synthesized, the reactivity of these complexes has been barely addressed. In particular, reactions under the preservation of the silyl–metal bond are rare. The reaction of the yttrium complex 2Y with NaCp is thus extremely promising as it highlights clean replacement of chlorides for cyclopentadienyl ligands to give 3 (Scheme 1).
Similarly, Liddle, Mills and co-workers used a substituted methane diide ligand system, which also features additional donor sites. Reaction of yttrium iodide complex 4 with alkali silanides gave the Y complexes 5, 6, and 7 with attached SitBu3, SitBu2Me, and Si(SiMe3)3 groups, respectively (Scheme 2).12
Shortly after this, Bart and co-workers demonstrated that the mentioned 1,5-oligosilanylene diide ligand 1 can also be used in actinide chemistry. They were able to prepare the first disilylated uranium(III) complex (2U) by reacting 1 with UI3 (Scheme 1).16 Later, they reported on the reactivity of 2U with aryl diazenes, which results in the formal insertion of aryl imido units into the Si–U bonds.17
Reviewing the organometallic chemistry of the lanthanides, it becomes evident that the number of homoleptic neutral trialkylated complexes is rather small.22 Although examples of Ln{CH(SiMe3)2}323–25 and Ln(CH2Ph)3(THF)3
26,27 are known, also these can suffer from ligand-dissociation caused instability. For this reason, it seemed not surprising that there were also no examples of homoleptic neutral trisilylated complexes known. However, recently Réant et al. were able to present first examples of this previously elusive class of compounds.
Already in 2014 Sgro and Piers had reported the reactions of the THF adducts of YI3 and GdI3 with (Me3Si)3SiK to proceed to (Me3Si)3SiYI2(THF)3 and (Me3Si)3SiGdI2(THF)3, respectively.28 Attempts to obtain di- or even trisilylated complexes were not mentioned in the study. Nevertheless, utilizing a similar approach, formation of the trisilylated complexes of La, Ce, Pr, Nd, and U (17M) by reacting three equivalents of (Me3Si)3SiK with the respective triodides was reported (Scheme 3).29
These compounds are quite unique. They constitute the first ever known examples of trisilylated f-element complexes and show most unusual properties with respect to their receptivity to NMR spectroscopic characterization. As mentioned, the detection of NMR signals of silylated f-element complexes is frequently hampered by their paramagnetism. However, for compounds 17M29Si NMR chemical shift values for the metal bound silicon atoms could be detected for all (i.e. also the paramagnetic Ce, Pr, Nd, and U) complexes. An alignment of the most magnetic axis along the three-fold rotation axis occupied by the coordinated THF molecules seems responsible for this unexpected behavior. The metal-bound silicon atoms and also the trimethylsilyl groups are thus not much affected (see Fig. 1 for calculated magnetic axes of complex 17Ce). The chemical shift value of diamagnetic [(Me3Si)3Si]3La(THF)3 (17La) in solution (C6D6/C4D8O: 9/1) was found to be −82.3 ppm. The fact that the respective values of paramagnetic [(Me3Si)3Si]3M(THF)2 (M = Ce, Pr, Nd, and U) were all observed within a small spectral window between −65.5 and −79.4 ppm, indicates how effective the suppression of the paramagnetic influence for this particular geometry is. CASSCF-SO-calculations were used to obtain a suitable model of the magnetic susceptibility tensor and to model the pNMR shifts of the paramagnetic 17M complexes for 0, 1, and 2 coordinated THF molecules.29
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Fig. 1 CASSCF-SO-calculated magnetic axes for 17Ce (blue: g1, most magnetic; green: g2, intermediate; red: g3, least magnetic) for complexes. Metal, silicon, carbon, and hydrogen atoms shown as metallic green, orange, gray, and light gray, respectively (figure reproduced from ref. 29). |
Layfield and co-workers reported the first erbium COT silole and stannole complexes.35 Reacting a COT [BH4] [THF]2 erbium complex with the same 2,5-bis(trimethylsilyl)silole dianion used by Roesky in 1,4-dioxane gave the anionic complex 22Er, which is monomeric in the solid state (Scheme 5).35 Investigations of the magnetic properties of the respective silole, stannole35 and germole36 erbium complexes revealed them as single-molecule magnets.
Complex | Si–M (Å) | δ Si (Si–M) (ppm) | Complex | Si–M (Å) | δ Si (Si–M) (ppm) |
---|---|---|---|---|---|
a Solid state CP/MAS 29Si NMR data. b Tentatively assigned. | |||||
2Y![]() |
3.064(2)/3.057(1) | −161.6 |
12Yb![]() |
2.9389(13) | n.d. |
2Ce![]() |
3.144(2)/3.159(2) | n.d. |
13La![]() |
3.1860(15) | −21.1a |
2Pr![]() |
3.119(2)–3.167(2) | n.d. |
13Ce![]() |
3.1705(9) | n.d. |
2Sm![]() |
3.089(2)/3.099(2) | n.d. |
14Lu![]() |
2.982(2)/2.9162(17) | n.d. |
2Tb![]() |
3.073(2)/3.081(2) | n.d. |
15Yb![]() |
3.060(3) | 54.2 |
2Dy![]() |
3.077(3)/3.077(3) | n.d |
15Eu![]() |
3.258(4) | n.d. |
3Y![]() |
3.1315(9)/3.1459(9) | −153.4 |
15Sm![]() |
3.261(3) | n.d. |
2U![]() |
3.1149(6)–3.1713(14) | n.d. |
16Yb![]() |
3.0678(14) | 29.2 |
5Y![]() |
3.062(2) | 33.5 |
16Eu![]() |
3.2075(9) | n.d. |
6Y![]() |
3.017(10) | 12.9 |
16Sm![]() |
3.2196(10) | n.d. |
7Y![]() |
3.0126(7) | −148.5 |
17La![]() |
3.197(3) | −82.3 |
8Th![]() |
3.1053(13) | −66.3 |
17Ce![]() |
3.172(2) | −79.4 |
9U![]() |
3.116(2) | n.d. |
17Pr![]() |
3.161(3) | −65.5 |
9La![]() |
3.178(2) | −130.3b |
17Nd![]() |
3.131(2) | −71.6 |
9Ce![]() |
3.153(2) | n.d. |
17U![]() |
3.114(2) | −70.5 |
9Nd![]() |
3.112(2) | n.d. |
18Eu![]() |
3.3276(10)/3.3294(9) | n.d. |
10La![]() |
3.1897(10) | −36.0a |
18Yb![]() |
3.2431(5)/3.1881(6) | 64.6 |
10Ce![]() |
3.1446(16) | n.d. |
19Eu![]() |
3.2309(6) | n.d. |
11La![]() |
3.1846(6) | −1.7a |
19Yb![]() |
3.0766(7) | 14.3 |
11Ce![]() |
3.1446(16) | n.d. |
20Y![]() |
3.0134(5) | 9.4 |
12La![]() |
3.1733(4) | 7.0a |
20La![]() |
3.1868(8) | 14.7 |
12Ce![]() |
3.1415(6) | n.d. |
20Lu![]() |
2.9380(7) | 27.9 |
12Sm![]() |
3.0729(7) | n.d. |
21La![]() |
3.0888(5) Si/3.2908(6) Si′ | 187.9 |
12Tb![]() |
3.0277(7) | n.d. |
22Er![]() |
2.882(2) | n.d. |
12Dy![]() |
3.0092(7) | n.d. |
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