Synthesis and characterisation of a novel europium-based graphite intercalation compound

In the lithium-europium-graphite system, a novel ternary compound was synthesised by direct immersion of a pyrolytic graphite platelet in a molten lithium-based alloy with a well chosen Li/Eu ratio at 400 °C. The ternary compound exhibits poly-layered intercalated sheets mainly constituted of two europium planes. Its chemical formula can be written Li_xEuC₄, since the amount of lithium is still not determined. The ¹⁵¹Eu Mössbauer spectra clearly indicate a +II valence for europium. The magnetic susceptibility and the magnetisation versus temperature reveal a complex behaviour which is qualitatively described thanks to structural hypothesis and analogies with the magnetic properties of the binary EuC₆ compound. A first ferromagnetic transition occurring at 225 K is attributed to interactions between both intercalated europium planes. The lower temperature susceptibility behaviour can be interpreted by antiferromagnetic interactions between in-plane neighbours and ferromagnetic interactions along the c-axis.     

六方氮化硼与石墨在形成层间化合物上的差异的理论研究

根据量子化学密度泛函B3LYP方法的计算结果,从六方氮化硼(h-BN）与石墨的前线轨道能级和两对离子探针（C^ 和C^-）的作用能所表现出来的在电亲和性上的差异以及金属层间化合物的电子结构,分析了h-BN不能形成金属层间化合物的原因。     

Facile sonochemical synthesis of graphite intercalation compounds

[reaction: see text] Graphite intercalation compounds (GICs) are useful as powerful reducing agents in organic chemistry and are typically prepared by anaerobic solid-state reactions at high temperatures for 1-8 h. We have been able to prepare KC(8) in situ in toluene using ultrasound in less than 5 min. This allows for a convenient approach to reductive chemical syntheses involving GICs.     

X-ray photoelectron study of fluorinated graphite intercalation compounds

Intercalated compounds of fluorinated graphite C₂F·yR, where R is benzene, hexafluorobenzene, acetone, or germanium tetrachloride, are studied by X-ray photoelectron spectroscopy. The binding energies of the C1s and F1s inner levels indicate that the C-F chemical bond in fluorinated graphite differs dramatically from the covalent bond in graphite monofluoride. The binding energies of the inner levels in atoms of the graphite fluoride matrix and GeCl₄ are analyzed and it is concluded that there is no chemical binding between the host matrix and the guest molecule. Translated fromZhurnal Struktumoi Khimii, Vol. 39, No. 6, pp. 1127–1133, November–December, 1998.     

Facile preparation of graphite intercalation compounds in alkali solution

Graphite intercalation compounds are often prepared by flake graphite, oxidants, inorganic acids, organic acids and intercalated ions which are usually hydrogen protons between the graphene planes. They are also known as the acid-treated graphite intercalation compounds. In this work, alkaline graphite intercalation compounds were prepared by flake graphite, K₂Cr₂O₇, concentrated H₂SO₄ and NaOH, and the morphology and structure were characterized by Electron microscopy and X-ray techniques. The results display that the combination of neutralisation heat and oxidation capability produced by K₂Cr₂O₇ can break the bonds to produce the spaces between the graphene planes and hydroxyl ions also intercalate into the graphene planes to form alkaline graphite intercalation compounds in alkali solution. The morphology and structure of alkaline graphite intercalation compounds are analogous to the ones of the acid-treated graphite intercalation compounds, but the intercalated ions and the expansion volume are different. The results show that the method is an innovation.     

Acceptor-type graphite intercalation compounds and new carbon materials based on them

The problems of synthesis and study of the physicochemical properties of graphite intercalation compounds (GIC) formed upon insertion of various molecules into the interplanar space of graphite are considered. Binary and ternary intercalation compounds with protonic acids (HNO₃, CH₃COOH, H₃PO₄, H₂SO₄, etc.) are described. The results of systematic research into graphite intercalation by potentiometry, calorimetry, powder X-ray diffraction, conductivity measurements, DTA, chemical analysis, and other methods are given. These results underlie elucidation of the characteristic and peculiar features of acid insertion into graphite. The physicochemical properties and practical applications of GIC and low-density carbon materials are analyzed. __________ Published in Russian in Izvestiya Akademii Nauk. Seriya Khimicheskaya, No. 8, pp. 1699–1716, August, 2005.     

Fe/膨胀石墨插层复合物的简易制备与电磁特性研究

以膨胀石墨和硫酸亚铁为前驱物,采用一步还原法得到Fe/膨胀石墨(Fe/EG)插层复合物.并用SEM、XRD、网络矢量分析仪等测试仪器分别研究了Fe含量(wFe)对Fe/EG插层复合物的形貌、结构、微波电磁和吸波性能的影响.结果表明:改变插层剂Fe的含量能有效地调控Fe/EG插层复合物的微波电磁与吸收特性.随wFe在27.5wt%～71.5wt%范围内增大,Fe/EG插层复合物的介电常数在wFe=27.5wt%时达到最大值,磁导率呈现多重共振现象,微波吸收性能逐渐增强.这种优异的微波吸收特性归功于Fe/EG插层复合物增强的电磁匹配和磁共振损耗.     

Thermal behaviour of graphite intercalation compounds with oxide of difluoride of phosphoryl

We present in this paper the thermal analysis (calorimetry, TG and DSC) of the first stage P₂O₃F₄ graphite intercalate compound in atmospheric pressure and high pressure. By heating we obtain always exfoliation phenomenon. The heating of exfoliated, graphite shows an important oxidation resistance in comparison with another exfoliated graphite. This oxidation resistance has been studied also by thermal analysis like TG, in oxygen atmosphere. Carbon foil rebuilding from exfolied graphite keeps these interesting antioxidation properties.     

Analogies and differences between two ways to evaluate the global hardness

The weight of the energetic components (electronic kinetic, electron-nucleus and electron-electron Coulombic, and correlation energies) of the ionization potential, electron affinity, chemical potential, and global hardness is evaluated and contrasted with the energetic components of the hardness kernel and the experimental values of these properties for 40 systems. The contrast of the hardness terms obtained from finite difference and hardness kernel gives some insight on the possible implications to differentiate the electronic energy with respect to the number electrons or the electron density.     

Synthesis of ternary and quaternary graphite intercalation compounds containing alkali metal cations and diamines

A series of ternary graphite intercalation compounds (GICs) of alkali metal cations (M = Li, Na, K) and diamines [EN (ethylenediamine), 12DAP (1,2-diaminopropane), and DMEDA (N,N-dimethylethylenediamine)] are reported. These include stage 1 and 2 M-EN-GIC (M = Li, d(i) = 0.68-0.84 nm; M = Na, d(i) = 0.68 nm), stage 2 Li-12DAP-GIC (d(i) = 0.83 nm), and stage 1 and 2 Li-DMEDA-GIC (d(i) = 0.91 nm), where d(i) is the gallery height. For M = Li, a perpendicular-to-parallel transition of EN is observed upon evacuation, whereas for M = Na, the EN remains in parallel orientation. Li-12DAP-GIC and Li-DMEDA-GIC contain chelated Li(+) and do not show the perpendicular-to-parallel transition. We also report the quaternary compounds of mixed cations (Li,Na)-12DAP-GIC and mixed amines Na-(EN,12DAP)-GIC, with d(i) values in both cases between those of the ternary end members. (Li,Na)-12DAP-GIC is a solid solution with lattice dimensions dependent on composition, whereas for Na-(EN,12DAP)-GIC, the lattice dimension does not vary with amine content.     

Balance between reversible and irreversible processes during lithium intercalation in graphite

The effect of the measurements’ speed on reversible and irreversible processes occurring during intercalation and deintercalation of lithium in graphite out of a 1 M LiClO₄ solution in a propylene carbonate-dimethoxyethane mixture is studied by the chronopotentiometry and cyclic voltammetry methods. Dependence of reversible and irreversible capacity on the potential scan rate during potentiodynamic measurements is shown to be quite involved. Lithium diffusion coefficients in graphite are calculated by different methods.     

Ternary graphite intercalation compounds associating an alkali metal and an electronegative element or radical

Ternary graphite intercalation compounds associating an alkali metal and an electronegative element are described. The synthesis is more often realized in molten alkali metal media containing the associate electronegative element or radical in the adequate concentration. The intercalated sheets are systematically polylayered. The arrangement along c-axis and the in-plane structures are described. The physical properties of the compounds are precised.     

Theoretical model and experimental study of pore growth during thermal expansion of graphite intercalation compounds

Summary A new technique, which allows one to simultaneously follow the mass and volume of graphite intercalation compounds (GICs) during thermal transformation into expanded graphite, was developed. This enabled us to elucidate the mechanism for the thermal expansion of GICs and formulate a quantitative model for the process. Effective activation parameters of the thermal decomposition of new GICs were obtained by using non-isothermal kinetics procedure. Thermal decomposition was described as a break of intermolecular bonds followed by diffusion.     

Heavy alkali metal-arsenic alloy-based graphite intercalation compounds: Investigation of their synthesis and of their physical properties

Heavy alkali metal-arsenic alloys intercalate easily into graphite, leading to the formation of a new family of ternary graphite intercalation compounds (GICs). Pure phases formulated as MAsxC4s (M = K, Rb or Cs; s = stage; x ≤ 1) have been synthesized at the laboratory. This article aims to expose all physical measurements performed on these intercalation compounds to get an idea about their electronic properties.Electrical conductivity measurements have been performed both parallel and perpendicular to the basal planes, between 4.2 and 295 K. Room temperature resistivity values lie between 16 and 35 μΩ cm and the anisotropic resistivity takes a value of an order of magnitude of 10⁴. Dynamic magnetic susceptibility measurements, carried out at low temperature on some phases, showed that they do not exhibit superconducting transition up to 1.3 K. Raman spectroscopy investigation, which is a useful tool to study the electronic and the chemical stability of GICs, highlighted a significant up-shift of the G-band of the carbon intra-layer vibration frequency, compared to the pure graphite vibration mode. Undoubtedly, this is related to the electronic charge transfer established between graphite layers and intercalated species.     

Modeling the electronic structure of graphite intercalation compounds with lithium by metal complexes with polybenzene systems

The electronic structure of intercalation compounds obtained by inclusion of an alkali metal in graphite is considered using molecular complexes C₆H₆Li₂, (C₆H₆)₂Li, and (C₆H₆)₃Li₂ in the lowest energy states as examples. Modeling the electron distributions of the intercalates requires inclusion of metal d-orbitals in the basis set of AOs and rejection of purely ionic models. It was found that exclusion of the lithium d-AO from the basis set significantly increases the ionic character of the distributions. Moscow State University. Translated fromZhurnal Strukturnoi Khimii, Vol. 37, No. 3, pp. 450–457, May–June, 1996.     

Preparation and characterization of a tetrabutylammonium graphite intercalation compound

The intercalation of tetrabutylammonium (TBA) cations into graphite by cation exchange from a sodium-ethylenediamine graphite intercalation compound yields a single-phase first-stage product, C(44)TBA, with a gallery expansion of 0.47 nm. The gallery dimension requires an anisotropic "flattened" cation conformation.     

Mass spectrometry of graphite intercalation compounds of binary fluorides of xenon,xenon oxide tetrafluoride and arsenic pentafluoride

Thermal decomposition of the intercalates of XeF₆, XeF₄, XeOF₄ and AsF₅ in graphite has been studied using a molecular beam source mass spectrometer. The product of the hydrolysis of the intercalate of XeF₆ has also been examined. The species liberated at low temperatures (T < 150°C) may be either the ones originally intercalated (XeOF₄, AsF₅) or the next lower oxidation state (XeF₄ from XeF₆, and XeF₂ from XeF₄. At higher temperatures (200-400°C) the intercalated XeF₄, XeF₂ or XeF₄ attack the graphite lattice, and evolve large quantities of xenon, and subsequently fluorocarbons and/or carbonyl fluoride. In contrast, the intercalate of AsF₅ evolves AsF₅ as the dominant gas over most of the temperature range, with a much lower degree of fluorination of the graphite lattice. The hydrolysis product of the XeF₆ intercalate was similar to the intercalate of XeF₄, but the evidence indicates that the hydrolysis proceeded well beyond XeOF₄. The extent of attack upon the graphite lattice correlates well with the oxidizing or fluorinating ability of the intercalated compound.