Molecular structure of 1-methyl-1-fluoroquasisilatrane (2-methyl-2-fluoro-1,3-dioxa-6-aza-2-silacyclooctane)

The molecular structure of 1-methyl-1-fluoroquasisilatrane (2-methyl-2-fluoro-1,3-dioxa-6-aza-2-silacyclooctane) MeFSi(OCH₂CH₂)₂NH (I) is determined by single crystal X-ray diffraction at 100 K. The coordination polyhedron of the silicon atom in this molecule is a slightly distorted trigonal bipyramid with an NH group and a strongly electron-withdrawing fluorine atom in the axial positions, and two endocyclic oxygen atoms and a CH₃ group in three vertices of the equatorial plane. The axial angle N→SiF is 171°. The length of the transannular donor-acceptor bond N→Si (2.058 Å) is as small as in 1-fluorosilatrane. The axial bond F-Si (1.660 Å) is longer than that in 1-fluorosilatrane and tetrahedral silicon compounds.     

From the Lithium‐2‐anilide‐2‐fluoro‐1,3‐diaza‐2‐sila‐cyclopentene‐GaCl3 Adduct to 1,4,6‐Triaza‐5‐gallium‐7‐sila‐cyclo‐3‐heptene ‐ Experimental and Quantum‐chemical Results

The lithium salt (HC–NCMe₃)₂SiFNLiR ( 1 ) R = C₆H₃(2,6‐CHMe₂)₂ reacts with trichlorogallium under displacement of the lithium ion by GaCl₃ to give the adduct [(HC–NCMe₃)₂SiFN]^– [(GaCl₃)R·Li(thf)₄]⁺ ( 1 ). Compound 1 thermally loses LiCl and forms the bicyclic ring intermediates V and VI . Compound  VI adds the aniline H₂NC₆H₃(2,6‐CHMe₂)₂ and the unsaturated, seven‐membered ring compound –NCMe₃–CH₂–CH=NCMe₃GaCl₂–NR–SiFNHR– ( 2 ) is obtained. The addition is accompanied by an enamine‐imine‐tautomerism and proves the Lewis acid character of the silicon atom in an unknown 3‐center‐2‐electron interaction of one nitrogen atom with the silicon and gallium atoms. Quantum chemical calculations of the thermal isomerisation process and crystal structures of 1 and 2 are reported.     

Reaction of tetrafluorosilane with tris(2-hydroxyethyl)amine, tris(2-trimethylsiloxyethyl)amine and bis(2-trimethylsiloxyethyl)amine and its N-methyl derivative. 1,1-difluoroquasisilatranes

Reaction of tetrafluorosilane with tris(2-hydroxyethyl)-and tris(2-trimethylsiloxyethyl)amine results in formation of 1-fluorosilatrane and fluorosilatrane in 75 and 53% yield, respectively. Reaction of tetrafluorosilane with bis(2-trimethylsiloxyethyl)amine and its N-methyl derivative leads to the hitherto unknown 1,1-difluoroquasisilatranes (N → Si) F₂Si(OCH₂CH₂)₂NR (R = H, Me) containing donor-acceptor bond N → Si and pentacoordinate silicon atom. The structure of the synthesized compounds was proved by ¹H, ¹³C, ¹⁵N, ¹⁹F, ²⁹Si NMR and IR spectroscopy.     

Molecular and crystal structure of two phases of 1-fluorosilatrane. Specific features of the electron density distribution

Using X-ray diffraction the presence of two phases of 1-fluorosilatrane (FSa) is stated and the specific features of their spatial structure are studied. Phase transition occurs at 156–158 K and is characterized by low energy. In the low-temperature phase, four crystallographically independent molecules are ordered, while in the high-temperature phase one of two independent molecules has disordered carbon β-atoms. A quantum chemical analysis of crystal packing in the low-temperature FSa phase is performed. The estimated value of the coordination N→Si bond strength in the crystal is 29.2 kcal/mol. The charge distribution indicates the localization of valence electron density around the O₃SiF fragment.     

Synthesen und Charakteristika von Heterobimetallorganika des Siliciums mit dem 2‐(Dimethylaminomethyl)ferrocenyl‐Liganden FcN (η5‐C5H5)Fe[η5‐C5H3(CH2NMe2)]—

Syntheses and characteristics of the heterobimetalorganics of the silicon with the 2‐(dimethylaminomethyl)ferrocenyl ligand FcN (η⁵‐C₅H₅)Fe[η⁵‐C₅H₃(CH₂NMe₂)]^— The heterobimetallic lithiumorganyl [2‐(dimethylaminomethyl)ferrocenyl] lithium, LiFcN, reacts with silicon(IV)‐chlorid, SiCl₄, under the formation of heterobimetallic silicon(IV) organyl [(FcN)₃SiCl] ( 1 ). The heterobimetallic organosilanol [(FcN)₃SiOH] ( 2 ) is formed at hydrolysis of 1 . A detailed characterization of the defined compounds 1 and 2 was carried out by NMR‐ rsp. mass‐spectrometry and by crystal X‐ray analysis of 2 .     

The Synthesis of tert‐Butyl(dichloromethyl)bis(trimethylsilyl)silane and (Dibromomethyl)ditert‐butyl(trimethylsilyl)silane and their Reactions with Organolithium Derivatives

tert‐Butyl(dichloromethyl)bis(trimethylsilyl)silane ( 4 ), prepared by the reaction of tert‐butylbis(trimethylsilyl)silane with trichloromethane and potassium tert‐butoxide, reacted with 2,4,6‐triisopropylphenyllithium (TipLi) (molar ratio 1 : 2) at room temperature to give (after hydrolytic workup) the silanol tBu(2,4,6‐iPr₃C₆H₂)Si(OH)–CH(SiMe₃)₂ ( 15 ). The formation of 15 is discussed as proceeding through the indefinitely stable silene tBu(2,4,6‐iPr₃C₆H₂)Si=C(SiMe₃)₂ ( 13 ), but attempts to isolate the compound failed. Treatment of (dibromomethyl)ditert‐butyl(trimethylsilyl)silane ( 7 ), made from tBu₂(Me₃Si)SiH, HCBr₃ and KOtBu, with methyllithium (1 : 3) at –78 °C afforded tBu₂MeSi–CHMeSiMe₃ ( 19 ); 7 and phenyllithium (1 : 3) under similar conditions gave tBu₂PhSi–CH₂SiMe₃ ( 20 ). The reaction paths leading to 15 , 19 and 20 are discussed. Reduction of 7 with lithium in THF produced the substituted ethylene tBu₂(Me₃Si)SiCH=CHSitBu₂SiMe₃ ( 21 ). For 21 the results of an X‐ray structural analysis are given.     

Novel Catalytic Hydrogenolysis of Trimethylsilyl Enol Ethers by the Use of an Acidic Ruthenium Dihydrogen Complex

The heterolytic cleavage of H ₂ is the key to the novel catalytic hydrogenolysis of trimethylsilyl enol ethers catalyzed by [RuCl(η²-H₂)(dppe)₂]OTf (dppe = 1,2-bis(diphenylphosphanyl)ethane, OTf = trifluoromethanesulfonate), which results in the formation of a ketone and Me₃SiH (see scheme). In addition, the stoichiometric, ruthenium-assisted protonation of a prochiral lithium enolate with H₂ gave a chiral ketone with high enantioselectivity (up to 75 % ee).     

LiLa5Si4N10O and LiPr5Si4N10O – Chain‐Type Oxonitridosilicates

The isotypic lithium rare‐earth oxonitridosilicates LiLn₅Si₄N₁₀O (Ln = La, Pr) were synthesized at temperatures of 1200 °C in weld shut tantalum ampoules employing liquid lithium as flux. Thereby, a silicate substructure with a low degree of condensation was obtained. LiLa₅Si₄N₁₀O crystallizes in space group P$\bar{1}$ [Z = 1, LiLa₅Si₄N₁₀O: a = 5.7462(11), b = 6.5620(13), c = 8.3732(17) Å, α = 103.54(3), β = 107.77(3), γ = 94.30(3), wR₂ = 0.0405, 1315 data, 96 parameters]. The nitridosilicate substructure consists of loop branched dreier single‐chains of vertex sharing SiN₄ tetrahedra. Lattice energy calculations (MAPLE) and EDX measurements confirmed the electrostatic bonding interactions and the chemical compositions. The ⁷Li solid‐state MAS NMR investigation is reported.     

Synthesis of fluoro-substituted atranes using MO2 oxides (M = Si, Ge, or Ti)

A new method for dissolving silicon, germanium, and titanium dioxides via the interaction with HF ? TEA (TEA stands for triethanolamine) yielding 1-fluorosilatrane, 1-fluorogermatrane, and 1-fluorotitanatrane, respectively, is proposed.     

Experimental Charge Density Studies of Cyclotetrasilazane and Metal Complexes Containing the Di‐ and Tetraanion

The homologous series of parent octamethylcyclotetrasilazane (c‐NH‐SiMe₂‐)₄, ( 1 ), the lithium complex [(THF)₂Li₂(c‐N‐SiMe₂‐NH‐SiMe₂‐)₂]₂, ( 2 ), containing the cyclic dianion, and [(THF)₂LiAl(c‐N‐SiMe₂‐)₄]₂, ( 3 ), accommodating the unprecedented tetraanion [Me₂SiN]^4‐ was synthesized to investigate the nature of the covalent Si‐N single bond in the presence of various metals. These model compounds show a wide diversity of Si‐N(H), Si‐N(M), Si‐N(H, M) and M‐N bonds and serve as bench‐mark systems to study polar bonds by high‐resolution low‐temperature X‐ray structure analysis. Experimental charge density studies reveal highly polar Si‐N bonds with remarkable ionic contribution, even in the non‐metallated starting material 1 . The Li‐N and Li‐O bonds have to be classified as almost purely ionic bonds with topological properties not far from those determined for NaCl.     

The structure of 1-chlorosilatrane: An ab initio molecular orbital and a density functional theory study

The molecular geometries of the 1-chloro-, 1-fluoro-, 1-methyl-, and 1-hydrogenosilatranes were fully optimized by the restricted Hartree-Fock (HF) method supplemented with 3-21G, 3-21G(d), 6-31G(d), and CEP-31G(d) basis sets; by MP2 calculations using 6-31G(d) and CEP-31G(d) basis sets; and by GGA-DFT calculations using 6-31G(d5) basis set with the aim of locating the positions of the local minima on the energy hypersurface. The HF/6-31G(d) calculations predict long (>254 pm) and the MP2/CEP calculations predicted short (∼225 pm) equilibrium Si(SINGLE BOND)N distances. The present GGA-DFT calculations reproduce the available gas phase experimental Si(SINGLE BOND)N distances correctly. The solid phase experimental results predict that the Si(SINGLE BOND)N distance is shorter in 1-chlorosilatrane than in 1-fluorosilatrane. In this respect the HF results show a strong basis set dependence, the MP2/CEP results contradict the experiment, and the GGA-DFT results in electrolytic medium agree with the experiment. The latter calculations predict that 1-chlorosilatrane is more polarizable than 1-fluorosilatrane and also support a general Si(SINGLE BOND)N distance shortening trend for silatranes during the transition from gas phase to polar liquid or solid phase. The calculations predict that the ethoxy links of the silatrane skeleton are flexible. Consequently, it is difficult to measure experimentally the related bond lengths and bond and torsion angles. This is the probable origin of the surprisingly large differences for the experimental structural parameters. On the basis of experimental analogies, ab initio calculations, and density functional theory (DFT) calculations, a gas phase equilibrium (r_e) geometry is predicted for 1-chlorosilatrane. The semiempirical methods predict a so-called exo minimum (at above 310 pm Si(SINGLE BOND)N distance); however, the ab initio and GGA-DFT calculations suggest that this form is nonexistent. The GGA-DFT geometry optima were characterized by frequency analysis. © 1996 by John Wiley & Sons, Inc.     

Lithiated Stannasilanes – Building Blocks for Monocyclic Si–Sn Rings

Dilithiated di(stannyl)oligosilanes (^tBu₂Sn(Li)– (SiMe₂)_n–Sn(Li)^tBu₂; 4 , n = 2; 5 , n = 3) were synthesized by the reaction of lithium diisopropylamide (LDA) with the α,ω‐hydrido tin substituted oligosilanes (^tBu₂Sn(H)– (SiMe₂)_n–Sn(H)^tBu₂; 1 , n = 2; 2 , n = 3). Surprisingly, the reaction of 1 and 3 (^tBu₂Sn(H)–(SiMe₂)₄–Sn(H)^tBu₂) with LDA resulted not in the formation of the lithiated compound, but what one can find is the formation of the 5,5‐ditert.butyl‐octamethyl‐1,2,3,4‐tetrasila‐5‐stannacyclopentane ( 8 ) (n = 4) in addition to the expected product 4 (n = 4) and the 3,3,6,6‐tetratert.butyl‐octamethyl‐1,2,4,5‐tetrasila‐3,6‐distannacyclohexane ( 7 ) (n = 3). Reactions of 4 and 5 with dimethyl and diphenyldichlorosilanes yielding monocyclic Si–Sn derivatives ( 9 – 11 ) are also discussed. The solid‐state structures of 7 and 11 were determined by X‐ray crystallography.     

Si–O-Bindungsspaltung in einem Siloxamin durch Aluminiumhydrid

Si–O Bond Fission in a Siloxamine by Aluminium Hydride When the alkoxyaminosilane tBu-O[tBuN(H)]SiMe₂ ( 1 ) reacts with aluminium hydride the expected cyclic alkoxyaluminosilane tBuO(tBuN)(AlH₂)SiMe₂ ( 2 ) is not obtained. Instead 1 reacts directly with two equivalents of aluminiumhydride to the alkoxyaminodialane 3 , (tBuO)(AlH₂)[N(SiMe₂H)tBu](AlH₂). The compound 3 is characterized by spectroscopic methods and by a single crystal X-ray diffraction analysis: the molecule has a four-membered OAl₂N cycle (Al–O 1.817(2) Å, Al–N 1.970(1) Å) as central unit. On the oxygen and nitrogen atom a tertbutyl or a tert-butyl and HMe₂Si group are attached, while the aluminium atoms have exclusively hydrogen as further ligands. The Si–O bond in the starting compound 1 has thus been cleaved, the oxygen atom being coordinated by aluminium and the silicon atom by hydrogen.     

The Synthesis and Molecular Structure of the First Two-Coordinate,Dinuclear σ-Bonded Mercury(I) RHgHgR Compound

A linear Si-Hg-Hg-Si arrangement and a Hg–Hg distance of 265.69 pm are exhibited by the first two-coordinate, dinuclear σ-bonded organomercury(I ) compound 1. It was formed unexpectedly in the reaction of two equivalents of the silane (Me₃SiMe₂Si)₃SiH with tBu₂Hg. In contrast if the reagents are allowed to react in a 1:1 ratio the expected mercury(II ) compound (Me₃SiMe₂Si)₃SiHgtBu is obtained.     

Quantum-chemical study of reaction mechanism between tris(2-hydroxyethyl)ammonium fluoride and tetraethoxysilane

DFT(B3LYP) analysis of thermodynamic stability of tris(2-hydroxyethyl)ammonium fluoride was carried out and its possible isomeric structures were localized. The potential surface of interaction of the found isomeric forms with tetraethoxysilanes was studied. Optimal gradient channel of formation of 1-fluorosilatrane was localized.     

Inhibition of lithium dendrites and dead lithium by an ionic liquid additive toward safe and stable lithium metal anodes

The uncontrolled growth of lithium dendrites and accumulation of “dead lithium” upon cycling are among the main obstacles that hinder the widespread application of lithium metal anodes. Herein, an ionic liquid (IL) consisting of 1-methyl-1-propylpiperidinium cation (Pp₁₃⁺) and bis(fluorosulfonyl)imide anion (FSI^?), was chosen as the additive in propylene carbonate (PC)-based liquid electrolytes to circumvent the shortcoming of lithium metal anodes. The optimal 1% Pp₁₃FSI acts as the role of electrostatic shielding, lithiophobic effect and participating in the formation of solid electrolyte interface (SEI) layer with enhanced properties. The in-situ optical microscopy records that the addition of IL can effectively inhibit the growth of lithium dendrites and the corrosion of lithium anode. This study delivers an effective modification to optimize electrolytes for stable lithium metal batteries.     

Low Concentration Sulfolane-Based Electrolyte for High Voltage Lithium Metal Batteries

Electrolyte engineering is crucial for the commercialization of lithium metal batteries. Here, lithium metal is stabilized in the highly reactive sulfolane-based electrolyte under low concentration (0.25 M) for the first time. Inorganic-polymer hybrid solid electrolyte interphase (SEI) with high ionic conductivity, low bonding with lithium and high flexibility enables dense chunky lithium deposition and high plating/stripping efficiency. Low concentration electrolyte (LCE) also enables excellent cycling stability of LiNi_0.5Co_0.2Mn_0.3O₂ (NCM523)/Li cells at 1 C (90.7 % retention after 500 cycles) and 0.3 C (83.3 % retention after 1000 cycles). With a low N/P ratio (≈2), the capacity retention for NCM523/Li cells can achieve 94.3 % after 100 cycles at 0.3 C. Exploring the LCE is of paramount significance because it provides more possibilities of the lithium salt selections, especially reviving some lithium salts that are excluded before due to their low solubility. More importantly, LCE has the significant advantage of commercialization due to its cost-effectiveness.     

流变相法制备倍率性能优异的LiFePO4/C复合材料

以月桂酸为碳源和表面活性剂,氢氧化锂、碳酸锂和醋酸锂为锂源,采用流变相法制备LiFePO4/C复合材料。运用X射线衍射(XRD)、扫描电子显微镜(SEM)、粒度分析、恒流充放电测试、循环伏安以及交流阻抗测试等方法对复合材料进行表征。结果表明,不同的锂源对LiFePO4/C复合材料的结构和电化学性能均有很大影响,以氢氧化锂为锂源合成的LiFePO4/C材料展示出最佳的循环性能和倍率性能。该材料在0.1C下放电比容量为153.4 mAh.g-1,在大倍率10 C下,容量保持率仍可达76%,甚至10C下循环800次后,容量衰减率仅有4%,SEM结果显示该材料具有较小的粒径(～200 nm),且分布集中,有效提高了电子迁移速率,从而改进了LiFePO4/C的倍率性能。     

Lithiumsalze des Tris(trimethylsilylamino)silans - Zur Struktur in Lösung und im Festkörper

Lithium Salts of Tris(trimethylsilylamino)silane - Their Structures in Solution and in the Solid State^* Amides, which result from the reaction of tris(trimethylsilylamino)silane (Me₃SiNH)₃SiH ( 1 ) with n-butyllithium in the molar ratio 1:1 and 1:2 in nonpolar solvents, form a system in which the aminosilane 1 , the monoamide (Me₃SiNLi)(Me₃SiNH)₂SiH ( 2a ), the diamide (Me₃SiNLi)₂(Me₃SiNH)SiH ( 3 ), and the triamide (Me₃SiNLi)₃SiH ( 4 ) are in equilibrium. When the monoamide 2a is dissolved in THF only the dimeric monolithiated THF adduct 2b is obtained. An X-ray structure analysis of the lithium silylamide 2b reveals that in the dimeric unit one of the lithium atoms is coordinated by THF, the two lithium atoms thus differing in coordination number (3 versus 4). An X-ray study of the triamide 4 reveals a centrosymmetric polycycle. Multipole interactions are formed between the lithium and the nitrogen atoms. The reaction of the diamide 3 with chlorotrimethylsilane in boiling THF yields the cis isomer of the cyclic diamide [(Me₃SiNLi)(Me₃SiNH)SiN(SiMe₃)]₂· 2 THF ( 5 ) as a byproduct. According to an X-ray structure analysis of 5 the lithium centers are coordinated by one oxygen and three nitrogen atoms, which form a strongly distorted tetrahedron. The interactions between lithium and nitrogen atoms N(1) and N(2), which are part of the four-membered Si₂N₂ cycle, have to be considered as weak on the basis of the remarkably long Li-N distances (233 and 243 pm).     

Reversible Lithium Intercalation into the Three‐Dimensional Cluster Network Structure of Ta6Cl15

A crystalline powder of Ta₆Cl₁₅ was synthesized through solid state reaction of Ta powder, and TaCl₅ at 700 °C. The structure contains [Ta₆Cl₁₂]³⁺ clusters which are three‐dimensionally interconnected by Cl bridges, leaving cavities which are shown to be suitable for lithium insertion. Reversible lithium intercalation into Ta₆Cl₁₅ involves 1 mol of lithium per formula unit under equilibrium conditions, when cells are discharged between 3 and 1.8 V, leading to the upper composition LiTa₆Cl₁₅. Although capacity values within this reversible voltage range are small (ca. 25 Ah·kg^?1), the cycle life of such Li/Ta₆Cl₁₅ cells is excellent, and the initial capacity value is maintained over 1500 cycles. On the other hand, a maximum of 15 moles of lithium can be reacted with one mole Ta₆Cl₁₅ when lithium cells were deep‐discharged. This process is likely due to the complete and irreversible reduction of the parent by lithium.