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1.
Two novel lithium nickel boride polymorphs, RT‐LiNiB and HT‐LiNiB, with layered crystal structures are reported. This family of compounds was theoretically predicted by using the adaptive genetic algorithm (AGA) and subsequently synthesized by a hydride route with LiH as the lithium source. Unique among the known ternary transition‐metal borides, the LiNiB structures feature Li layers alternating with nearly planar [NiB] layers composed of Ni hexagonal rings with a B–B pair at the center. A comprehensive study using a combination of single crystal/synchrotron powder X‐ray diffraction, solid‐state 7Li and 11B NMR spectroscopy, scanning transmission electron microscopy, quantum‐chemical calculations, and magnetism has shed light on the intrinsic features of these polymorphic compounds. The unique layered structures of LiNiB compounds make them ultimate precursors for exfoliation studies, thus paving a way toward two‐dimensional transition‐metal borides, MBenes.  相似文献   

2.
The results of the X-ray structural study for the K4LiH3(SO4)4 single crystal are presented at a wide temperature range. The thermal expansion of the crystal using the X-ray dilatometry and the capacitance dilatometry from 8 to 500 K was carried out. The crystal structures data collection, solution and refinement at 125, 295, 443 and 480 K were performed. The K4LiH3(SO4)4 crystal has tetragonal symmetry with the P41 space group (Z=4) at room temperature as well as at the considered temperature range. The existence of a low-temperature, para-ferroelastic phase transition at about 120 K is excluded. The layered structure of the crystal reflects a cleavage plane parallel to (001) and an anisotropy of the protonic conductivity. The superionic high-temperature phase transition at TS=425 K is isostructural. Nevertheless, taking into account an increase of the SO4 tetrahedra libration above TS, a mechanism of the Grotthus type could be applied for the proton transport explanation.  相似文献   

3.
High-pressure X-ray diffraction measurements were carried out for polymeric CdI2-type compounds MTe2 (M=Pt, Pd) to investigate if they undergo a structural phase transition under pressure as does IrTe2. Up to 27 GPa at room temperature PtTe2 does not undergo any structural phase transition. In contrast, however, an abrupt change in the inter-atomic distances occurs in PdTe2 above 15.7 GPa at room temperature, and above 5 GPa at 300 °C, but the volume vs. pressure curve exhibits no discontinuity. To account for the differences between the isostructural compounds PtTe2, PdTe2 and IrTe2, their electronic structures and bonding were analyzed on the basis of first principles electronic band structure calculations.  相似文献   

4.
Crystal chemical indices of ion segregation and electrostatic imbalance after Beck help to rationalize inorganic crystal structures and sometimes even to predict them. Metal hydrides, from hydrido‐aluminates and ‐gallates, to complex transition metal hydrides, ternary ionic magnesium hydrides and mixed anionic hydrides, were investigated using these tools. Beck's ion segregation and electrostatic imbalance indices are found to work well in explaining crystal structures of most metal hydrides, although the electronegativity differences between cations and hydride anions are often much smaller in ionic metal hydrides, as compared to metal fluorides and oxides. This includes complex transition metal hydrides, despite the fact that formal oxidation states do not describe the actual charges properly. Rare cases of violations can be explained by the chemical bonding situation, e.g. the presence of weak metal–metal bonds in Li3RhH4.  相似文献   

5.
The phases TiRhSi, TiPdSi, MnRhSi, ZrFeGe, ZrRhGe, ZrPdGe, and NbRhGe crystallize with the TiNiSi (ordered anti-PbCl2) structure. ZrRuSi possesses the Fe2P structure, while TiRuSi has the closely related TiFeSi structure. Cell parameters for these phases and a refinement of the structure of ZrRuSi from X-ray powder data are reported. Relationships among the observed structural types as well as the “filled” NiAs (Ni2In) type are pointed out. The crystal chemistry of ternary equiatomic phases of two transition metals and silicon or germanium is discussed, emphasizing differences in metal-metal bonding.  相似文献   

6.
A series of binary rare-earth metal silicides RE5Si3 and ternary boron-interstitial phases RE5Si3Bx (RE=Gd, Dy, Ho, Lu, and Y) adopting the Mn5Si3-type structure, have been prepared from the elemental components by arc melting. Boron “stuffed” phases were subsequently heated at 1750 K within a high-frequency furnace. Crystal structures were determined for both binary and ternary series of compounds from single-crystal X-ray data: hexagonal symmetry, space group P63/mcm, Z=2. Boron insertion in the host binary silicides results in a very small decrease of the unit cell parameters with respect to those of the binaries. According to X-ray data, partial or nearly full boron occupancy of the interstitial octahedral sites in the range 0.6-1 is found. The magnetic properties of these compounds were characterized by the onset of magnetic ordering below 100 K. Boron insertion induces a modification of the transition temperature and θp values in most of the antiferromagnetic binary silicides, with the exception of the ternary phase Er5Si3Bx which was found to undergo a ferromagnetic transition at 14 K. The electrical resistivities for all binary silicides and ternary boron-interstitial phases resemble the temperature dependence of metals, with characteristic changes of slope in the resistivity curves due to the reduced electron scattering in the magnetically ordered states. Zintl-Klemm concept would predict a limiting composition RE5Si3B0.6 for a valence compound and should then preclude the stoichiometric formula RE5Si3B. Density functional theory calculations carried out on some RE5Si3Zx systems for different interstitial heteroatoms Z and different x contents from 0 to 1 give some support to this statement.  相似文献   

7.
The effects of feed composition on the adsorption dynamics and the optimal process design were studied from the experimental and simulated results in the H2 layered bed PSA with activated carbon and zeolite 5A. The breakthrough results using the base composition (56.4 vol% H2; 26.6 vol% CH4; 8.4 vol% CO; 5.5 vol% N2; and 3.1 vol% CO2) in various layered beds were compared with those using the higher nitrogen composition and the no nitrogen composition. In the breakthrough dynamics, the propagation velocity of wave front of each component was closely related to the slope of isotherm estimated at its concentration in the feed. Breakthrough behavior at each layered bed in the higher nitrogen composition showed similar trends as that in the base composition. However, the no nitrogen composition showed different breakthrough behavior from the other groups. In this feed composition, it was observed that the order of CO and CH4 breakthrough times was reversed with a change in the carbon-to-zeolite ratio. Based on the adsorption dynamics and breakthrough behavior of each feed composition group in various layered beds, the effect of feed composition on a seven-step two-bed PSA process for the H2 recovery from coke oven gas was investigated numerically to develop a well-designed H2 PSA process under various operating conditions. As expected from the breakthrough results, the trends of the PSA performance in the higher nitrogen composition were similar to those in the base composition except for the slight decrease in the optimal carbon-to-zeolite ratio. However, in case of the no nitrogen composition, high purity product was obtained from the activated carbon-rich layered bed PSA because the adsorption capacity of the activated carbon for impurities was superior to that of zeolite. As a result, the optimum carbon-to-zeolite ratio at each operating condition was slightly changed depending on the propagation velocity of each component on each layer.  相似文献   

8.
Uniform and sphere-like nanoparticles of crystalline Pr3+-doped CaTiO3 have been prepared from complex polymer precursor at 600°C, in which, metal atoms are previously dispersed by citric acid in ethylene glycol solvent. The decomposition process of the precursor, crystallization, and particle sizes of CaTiO3 have been investigated by using thermal analysis, powder X-ray diffraction and transmission electron microscopy. Diffuse reflectance spectra, photoluminescence and decay curve indicate that a strong red emission located at the nearly NTCS “ideal red” site is deduced from the energy transfer from the band gap absorption to doping Pr3+ ions. The thermoluminescence curves exhibit that a potential long phosphorescent material based on Pr3+-doped CaTiO3 will be explored in future.  相似文献   

9.
In situ neutron powder diffraction data have been analysed for a number of compositions in the solid solution series La2Ni1−xCoxOδ over the temperature range 150-650 °C. High-quality Rietveld refinements indicate no major structural transitions have occurred in any of the compositions, although close examination of the Ni/CoO bond distances highlight changes in the coordination environment with increasing temperature. Further, the changes in the coordination can be correlated to changes in both the oxide ion and electronic conductivity indicating a direct link between transport properties, bonding and transition metal valence state in these Co containing layered perovskites.  相似文献   

10.
Starting from the precursors containing active metal species in the crystal structure, highly dispersed supported metal catalysts have been prepared by the calcination-reduction treatment. This method is named as solid phase crystallization (spc) method and was compared with the conventional impregnation (imp) method. As the precursors, both perovskite-type and hydrotalcite-type oxides have been utilized for preparing various supported metal catalysts, which were successfully applied for the reforming of CH4 and the decomposition of methanol. Especially spc-Ni/Mg–Al catalyst prepared from the hydrotalcite-type precursors showed high activity as well as high sustainability for the hydrogen production from methane.  相似文献   

11.
The perovskite-related layered structure of La2Ti2O7 has been studied at pressures up to 30 GPa using synchrotron radiation powder X-ray diffraction (XRD) and Raman scattering. The XRD results indicate a pronounced anisotropy for the compressibility of the monoclinic unit cell. The ratio of the relative compressibilities along the [100], [010] and [001] directions is ∼1:3:5. The greatest compressibility is along the [001] direction, perpendicular to the interlayer. A pressure-induced phase transition occurs at 16.7 GPa. Both Raman and XRD measurements reveal that the pressure-induced phase transition is reversible. The high-pressure phase has a close structural relation to the low-pressure monoclinic phase and the phase transition may be due to the tilting of TiO6 octahedra at high pressures.  相似文献   

12.
Solid, polymer membranes fabricated from room-temperature ionic liquid monomers containing oligo(ethylene glycol) or nitrile-terminated alkyl substituents tethered to imidazolium cations were found to exhibit ideal CO2/N2 and CO2/CH4 separation factors significantly greater than those with comparable length n-alkyl substituents, with similar CO2 permeability. Polymers containing these functional groups exhibited CO2/N2 gas separation performance exceeding the “upper bound” of a “Robeson Plot”.  相似文献   

13.
Monodispersed AgGaS2 three-dimensional (3D) nanoflowers have been successfully synthesized in a “soft-chemical” system with the mixture of 1-octyl alcohol and cyclohexane as reaction medium and oleylamine as surfactant. The crystal phase, morphology and chemical composition of the as-prepared products were characterized by X-ray diffraction (XRD), transmission electron microscopy (TEM), and high-resolution TEM (HTEM), respectively. Results reveal that the as-synthesized AgGaS2 nanoflowers are in tetragonal structure with 3D flower-like shape. Controlled experiments demonstrated that the shape transformation of AgGaS2 nanocrystals from 3D nanoflowers (50 nm) to nanoparticles (10-20 nm) could be readily realized by tuning the reaction parameters, e.g., the ratio of octanol to cyclohexane, the length of carbon chain of fatty alcohol, the concentration of oleylamine, etc. The UV-vis and PL spectra of the obtained AgGaS2 nanoflowers and colloids were researched. In addition, the photoelectron energy conversion (SPV) of AgGaS2 nanoflowers was further researched by the surface photovoltage spectra.  相似文献   

14.
《Mendeleev Communications》2022,32(6):820-822
Synthesis of solid solutions of transition metal borides (NbB2, TaB2, HfB2 and ZrB2) and carbides (NbC, TaC, HfC, ZrC and VC) was carried out via sintering the individual components without applying pressure. To activate the interaction of the components, the initial powders were processed by high-energy shock wave treatment (HESWT). HESWT enables the formation of homogeneous solid solution for a mixture of carbides; however, this method did not give the desired results for a mixture of transition metal borides, likely due to the higher strength of borides crystal lattice in comparison with carbides.  相似文献   

15.
A general and efficient solvothermal strategy has been developed for the preparation of lithium transition metal phosphate microstructures (LiMnPO4, LiFePO4, and LiCoPO4), employing ethanol as the solvent, LiI as the Li source, metal salts as the M sources, H3PO4 as the phosphorus source, and poly(vinyl pyrrolidone) (PVP) as the carbon source and template. This route features low cost, environmental benign, and one-step process for the cathode material production of Li-ion batteries without any complicated experimental setups and sophisticated operations. The as-synthesized LiMPO4 microstructures exhibit unique, well-shaped and favorable structures, which are self-assembled from microplates or microrods. The b axis is the preferred crystal growth orientation of the products, resulting in a shorter lithium ion diffusion path. The LiFePO4 microstructures show an excellent cycling stability without capacity fading up to 50 cycles when they are used as a cathode material in lithium-ion batteries.  相似文献   

16.
采用溶胶凝胶法制备了V2O5-TiO2复合半导体材料,通过Raman、XRD及UV-Vis DRS等实验方法研究了V2O5与TiO2复合对材料表面组成、晶体结构以及光响应性能的影响。结果表明:钒加入后优先与TiO2作用形成较为稳定的金红石型TiVO4晶相,其中V4+是促进TiO2发生相变的关键;随着钒加入量的增加,V2O5由表面高分散状态逐渐聚集形成晶相,并释放部分Ti4+使之形成锐钛矿型TiO2晶相,使得体相中金红石型TiO2的含量有所下降;复合后形成的TiVO4晶相显著提高了材料对可见光的吸收率,并使其吸光域红移至460 nm左右。  相似文献   

17.
η2 π-Complexes of Ge2H2 with the organometallic fragments V(PH3)2(I)(CO)2, Cr(CO)4, Co(PH3)2(Cl) and M(PH3)2 (M = Ni, Pd, Pt) have been studied at the B3LYP level using the SBKJC relativistic effective core potentials and their associated basis sets on metals and iodine, and the 6-31G(d) basis set on all other elements. The transition metal fragments of V, Cr, Co, Ni, Pd and Pt were chosen based on known alkyne compounds. All the complexes are local minima for both the HGeGeH and GeGeH2 isomers of the Ge2H2 ligand. The complexes containing GeGeH2 isomer as a ligand are lower in energy than those with the HGeGeH ligand (except in the V complex in which the difference is only 1.0 kcal/mol). There is a net charge transfer from ligand to metal in complexes V-Co and from metal to ligand in late transition metal complexes (Ni-Pt).  相似文献   

18.
Summary In this work, we search for the simplest complete surfaces of systems with three and four atoms, i.e. the minimal sets of critical points with their index, which are topologically consistent in the whole configuration space. Then we show the smallest change in the A2B2 system by requiring at least one stable acetylene configuration and one stable vinylidene configuration, like on the C2H2 surface. Finally, we give complete sets of minima, saddle points and maxima obtained for C2H2 with analytical potentials proposed in the literature and with a semi-empirical method at the CAS-CI level.  相似文献   

19.
Reported are the syntheses, crystal structure determinations from single-crystal X-ray diffraction, and magnetic properties of two new ternary compounds, Eu11Cd6Sb12 and Eu11Zn6Sb12. Both crystallize with the complex Sr11Cd6Sb12 structure type—monoclinic, space group C2/m (no. 12), Z=2, with unit cell parameters a=31.979(4) Å, b=4.5981(5) Å, c=12.3499(14) Å, β=109.675(1)° for Eu11Zn6Sb12, and a=32.507(2) Å, b=4.7294(3) Å, c=12.4158(8) Å, β=109.972(1)° for Eu11Cd6Sb12. Their crystal structures are best described as made up of polyanionic and ribbons of corner-shared ZnSb4 and CdSb4 tetrahedra and Eu2+ cations. A notable characteristic of these structures is the presence of Sb-Sb interactions, which exist between two tetrahedra from adjacent layers, giving rise to unique channels. Detailed structure analyses shows that similar bonding arrangements are seen in much simpler structure types, such as Ca3AlAs3 and Ca5Ga2As6 and the structure can be rationalized as their intergrowth. Temperature-dependent magnetization measurements indicate that Eu11Cd6Sb12 orders anti-ferromagnetically below 7.5 K, while Eu11Zn6Sb12 does not order down to 5 K. Resistivity measurements confirm that Eu11Cd6Sb12 is poorly metallic, as expected for a Zintl phase.  相似文献   

20.
The fluorine-containing derivatives of Sr2MnGaO5.5 were prepared by treatment with XeF2 at temperatures ranging from 300°C to 600°C. The compounds crystallize in a tetragonal unit cell with atap, ct≈2ap (ap—the parameter of the perovskite subcell). An increase in fluorine content is accompanied by a reduction of the Mn oxidation state due to a partial replacement of oxygen by fluorine. The crystal structure of Sr2MnGaO4.78F1.22 was determined by electron diffraction and X-ray powder diffraction (a=3.85559(2) Å, c=7.78289(6) Å, S.G. P4/mmm, RI=0.012, RP=0.019). The structure consists of alternating (MnO2), (SrO) and (GaO0.78F1.22) layers. The Ga atoms are situated in slightly elongated octahedra, the MnO6 octahedra are characterized by two short apical Mn-O distances of 1.876(8) Å and four long equatorial ones of 1.9278(1) Å. This is interpreted as an “apically compressed” type of Jahn-Teller distortion, in contrast to the “apically elongated” one in the Sr2MnGaO5+δ brownmillerites with different oxygen content. Possible structural reasons for the reversed Jahn-Teller effect are discussed.  相似文献   

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