Lithium aluminum nitride,Li3AlN2 as a lithium solid electrolyte

Single phase of Li₃AlN₂ was prepared from the mixture of Li₃N/AlN = 1.2 to 1.5 in molar ratio at 700°C and at 900°C. It crystalizes in the cubic system derived from antifluorite-type structure having the lattice parameter $\text{a = 9.470}\text{A}\text{?}$. It is a pure ionic conductor having conductivity of 5 × 10^?8ω^?1cm^?1 at room temperature and an activation energy of 52 kJ/ mol. Its decomposition voltage was 0.85 V at 104°C. The TiS₂/Li₃AlN₂/Li cell could be discharged at a constant current of 45 μA/cm² at 104°C.     

Ionic conductivity of pure and doped Li3N

The ionic conductivity of Li₃N crystals doped with various metal ions (magnesium, copper and aluminum) or hydrogen has been investigated. The metal ions have a negative effect on the conductivity whereas hydrogen increases it. The intrinsic Li⁺ ionic conductivity of pure Li₃N is (2·-4)×10^-4Ω^-1cm^-1 at room temperature with an activation energy of 0.26?0.27 eV. Doping with hydrogen to a maximum level of 0.5?1.0 atom% results in a conductivity of 6×10^-3Ω^-1cm^-1 and an activation energy which has been lowered to 0.20 eV. A model is proposed for the action of hydrogen whereby the Li-N bonds next to an NH^2- group are weakened thereby facilatating the creation of Li⁺ Frenkel defects and the vacancy migration. Hydrogen-doped Li₃N is termed an enhanced intrinsic conductor.     

Li2Mo2O6多晶材料的结构与电性能的研究

本文用固相反应烧结制备出Li₂Mo₂O₆多晶材料。经X射线分析、红外光谱和电子顺磁共振谱(EPR)的研究,确定了它的结构是Li₂Mo₂O₄和MoO₂两个晶相组成的烧结体。钼离子以四价状态存在于MoO₂晶相结构中。采用交流阻抗谱分析了晶界与温度变化的相关性。测得了样品的ln(σ_总T)-1/T 曲线是由两段直线和一段曲线所组成;总电导率化能σ_27℃=1.36×10^-3(Ω·cm)^-1,σ_115℃=1.49×10^-3(Ω·cm)^-1,σ_300℃=9.71×10^-3(Ω·cm)^-1,σ_370℃=2.42×10^-3(Ω·cm)^-1;电导活化能E₁=0.043eV,E₂=0.235eV,E_平均=0.76eV。采用维格纳极化电池法测得电子电导率σ_e,σ_e27℃=2.240×10^-5(Ω·cm)^-1,σ_e300℃=4.476×10^-3(Ω·cm)^-1。实验证明,室温下材料为固体电解质,300℃附近为良好的离子与电子混合导体。 关键词：     

Li4SiO4-Li3VO4赝二元系和Li4GeO4-Li4SiO4-Li3VO4赝三元系中新的锂离子导体

本文在室温到300℃的温度范围内研究了Li₄SiO₄-Li₃VO₄和Li₄GeO₄-Li₄SiO₄-Li₃VO₄体系中的离子导电性,发现γ_II相固溶体Li_3+xV_1-xSi_xO₄是好的锂离子导体。所研究的成分中Li_3.3V_0.7Si_0.3O₄的离子电导率最高,室温下为1×10^-5Ω^-1·cm^-1,在42—192℃的电导激活能为0.36eV,电子电导率可以忽略,因而这是迄今所发现的最好的锂离子导体之一。粗略确定了Li₄GeO₄-Li₄SiO₄-Li₃VO₄三元系中电导率高的范围,发现在Li_3.5V_0.5Ge_0.5O₄中Si部分取代Ge可以使电导率进一步提高,Li_3.5V_0.5Ge_0.4Si_0.1O₄的室温电导率可达1.3×10^-5Ω^-1·cm^-1,电导激活能为0.40eV。 关键词：     

New Li+ ion conductors in the system Li4SiO4−Li3AsO4

In the system Li₄SiO₄-Li₃AsO₄, Li₄SiO₄ forms a short range of solid solutions containing up to 14 to 20% Li₃AsO ₄, depending on temperature, and γ-Li₃AsO₄ forms a more extensive range of solid solutions containing up to ≈55% Li₄SiO₄. The Li₄SiO₄-Li₃AsO₄ phase diagram has been determined and is of binary eutectic character. The ac conductivity of polycrystalline samples was measured over the range 0 to at least 300°C for nine different compositions. The two solid solution series have much higher conductivity than the pure end-members; maximum conductivity was observed in the γ-Li₃AsO₄ solid solutions containing ≈40 to 55% Li₄SiO₄, with values of $\text{≈2×10}{}^{\mathrm{?6}}\text{Ω}{}^{\mathrm{?1}}\text{cm}{}^{\mathrm{?1}}$ at 20°C rising to ≈0.02 Ω^?1 cm^?1 at 300°C. These values are comparable to those found in the system Li₄SiO₄-Li₃PO₄. The variation with composition of the Arrhenius prefactor and activation energy has been interpreted in terms of the mechanisms of conduction. Li₃AsO₄ is a poor conductor essentially because the number of mobile Li⁺ ions is very small. This number, and hence the conductivity, increases dramatically on forming solid solutions with Li₄SiO₄, by the creation of interstitial Li⁺ ions. At ≈40 to 55% Li₄SiO₄, the number of mobile Li⁺ ions appears to be optimised. An explanation for the change in activation energy of conduction at ≈290°C in Li₄SiO₄ and at higher temperatures in Li₄SiO₄ solid solutions is given in terms of order-disorder of the Li⁺ ions.     

Lithium ion conductors of polyion complexes dispersed with LiClO4 and their application to solid-state batteries

Polyion complexes between poly(sodium acrylate) $\text{2}$ and polybrene $\text{3}$, or poly(2-acrylamino-2-methylpropane sulfonate) $\text{2}$ and $\text{2}$ were synthesized. After removing sodium bromide, these polymers were dispersed with LiClO₄, and their Li⁺ conductivities were measured at 80 ～ 200°C. Their ionic conductivities changed from 10^-3 to 10^-8 S cm^-1 at 100 ～ 200°C. These polymers and poly(ethylene oxide) dispersed with LiBF₄ were used as solid electrolytes of Li-activated carbon fiber (ACF) batteries and ACF-ACF capacitor.     

多晶Li3+xV1-xTxO4(T=Ge,Si)离子导电性能的改善

本文用阻抗谱方法研究了Li_3+xV_1-xT_xO₄(T=Si,Ge)多晶的离子导电性,发现一些工艺条件如成型压强、烧结时间和烧结程序对电导率有很大影响。注意分析了这些影响的物理起因。最佳工艺条件是:在大约8t/cm²压强下成型样品。在1000℃连续烧结5至6天,烧结过程中,应尽量避免温度波动。在此条件下制备的Li_3.5V_0.5Ge_0.5关键词：     

Determination of A0 for CH335Cl and CH337Cl from the ν4 infrared and Raman bands

The ν₄ infrared and Raman bands of CH₃Cl were analyzed simultaneously. A direct fit yielded a complete set of constants for CH₃³⁵Cl, including A₀ = 5.20530 ± 0.00010 cm^?1 and D_K = (8.85 ± 0.13) × 10^?5cm^?1. For CH₃³⁷Cl an incomplete set of constants was obtained from the infrared band, and A₀ = 5.2182 ± 0.0010 cm^?1 was estimated by curve fitting of the Raman spectrum. The resulting equilibrium structure is $\text{r(}\text{CH) = 1.0854 ± 0.0005}\text{A}\text{?}$, $\text{r(}\text{CCl) = 1.7760 ± 0.0003}\text{A}\text{?}$, and <(HCH) = 110°.35 ± 0°.05.     

Ionic conductivity of substituted Li7TaO6 phases

Lithium ion conductivity in solid solutions of Li₇Ta_1-xNb_xO₆, Li₇Ta_1-xBi_xO₆, Li_7+xTa_1-xZr_xO₆ and Li_7-2xCa_xTaO₆ has been measured as a function of temperature and composition using the complex impedance method. At 200°C the conductivities of Li₇Ta_0.7Nb_0.3O₆, Li_7.4Ta_0.6Zr_0.4O₆ and Li_6.6Ca_0.2TaO₆ are 4.3 × 10^-4(ωcm)^-1, 3.0 × 10^-4(ωcm)^-1, 4.0 × 10^-4(ωcm)^-1 and 1.6 × 10^-4(ωcm)^-1 respectively. The results are discussed in relation to structural properties.     

LISICON(锗酸锌锂)单晶的Li+离子电导

本文研究了Lisicon(锗酸锌锂)单晶的Li⁺离子电导率。发现各结晶学方向电导率之间的关系为σ_b≤σ_a≤σ_c≤σ_[110],但各向异性不强。晶体中Li含量对电导率有明显的影响,当Li/Zn比率由6.7变到9.2时,300℃a方向电导率由4.3×10^-2Ω^-1·cm^-1增加到1.25×10^-1Ω^-1·cm^-1,logσT对1/T的曲线显示出三个转变点,分别在～80℃,～140℃和～300℃。电导的激活能分别为0.50—0.58eV(25—80℃),0.92eV(～80—140℃),0.64eV(～140—300℃)和0.36eV(>300℃),极化实验表明单晶的电子电导可以忽略。 关键词：     

插层化合物Li1+xV3O8的合成及其物理性能的初步研究

本文成功地合成了插层化合物Li_1+xV₃O₈,并用X射线粉末衍射和等离子体发射光谱元素定量分析进行了鉴定。同时进行了NMR研究。在298—400K之间观察到了锂离子的运动致窄效应,并以此求得它的离子运动激活能为0.18eV。还测得该材料的室温电导率为10^-3Ω^-1·cm^-1数量级。 关键词：     

Li2Mo2-xWxO6多晶材料的结构、电学性能与导电机理的研究

本文采用还原气氛制备导电性能优良的多晶多相陶瓷材料Li₂Mo_2-xW_xO₆(x=0,0.1,0.3),采用粉末X射线衍射分析、特征X射线能谱分析、红外光谱分析和电子自旋共振波谱分析等现代测试手段,得到样品的物相结构为Li₂Mo_1-xW_xO₄和MoO₂两相组成。W的掺入主要取代Mo进入Li₂ 关键词：     

Li2O-2B2O3熔体的物性研究

系统测量了四硼酸锂(Li₂Ｏ-２Ｂ_２Ｏ_３)熔体的密度ρ、表面张力γ随着温度的变化规律，实验结果表明在1100K到1500K范围内Li₂Ｏ-２Ｂ_２Ｏ_３高温熔体的密度和表面张力随着温度的升高均线性减小.通过实验数据拟合得出熔体密度与温度关系为ρ(T)=2.574—4.89×１０^－４T，熔点处Li₂Ｏ-２Ｂ_２Ｏ关键词： 功能晶体 四硼酸锂 密度 表面张力     

Characterization and electrical behavior of new lithium chalcoborate thin films

Thin films obtained with glasses of the B₂S₃Li₂S and B₂S₃Li₂SLiI systems, using a vacuum evaporation technique have been investigated. In each system, amorphous thin films and starting glasses have the same composition and similar conductivities, about 10^?4 and 10^?3Ω^?1cm^?1 respectively at 25°C. The deposition rate was in both cases 140 Å s^?1. However, a thermal treatment at 90°C of the thin films containing lithium iodide enhances the conductivity by a factor of 10 and leads to lower activation energy (0.18 eV). This behavior has been identified as a Phipps effect and can be attributed to a quick ion diffusion along thin film - substrate interface. This interfacial region was found to show unique conduction properties including a very low Li⁺ migration enthalpy.     

Li1+xGe2-xAlxP3O12系统的相关系和电导

本文研究了Li_1+xGe_2-xAl_xP₃O₁₂系统的相组成和电导的关系。发现用LiGe₂P₃O₁₂作为基体化合物,通过离子置换可以得到好的锂离子导体。用Al³⁺置换LiGe₂P₃O₁₂中的Ge⁴⁺,在0关键词：     

Preparation and structural studies of lithium substituted nickel phosphorus trisulphide,Li2NiP2S6

Crystals of Li₂NiP₂S₆ may be prepared by direct combination of stoichiometric amounts of Li₂S, phosphorus, nickel and sulphur in a temperature gradient towards 750°C. The structure determined by X-ray powder diffraction is monoclinic C2/m with $\text{a = 5.926}\text{A}\text{?}\text{, b = 10.917}\text{A}\text{?}\text{, c = 6.718}\text{A}\text{?}\text{, β = 104.4°}$, and is based on the NiPS₃ layer structure with two Ni atoms substituted by lithium, and with two lithium atoms in the van der Waals gap.     

Preparation and semiconducting properties of Th3As4

The resistivity, thermoelectric power and Hall constant in the temperature range of 78–830 K were determined for polycrystalline Th₃As₄ samples obtained by annealing thin thorium slabs in arsenic vapour. The samples examined were n-type semiconductors with a carrier concentration ranging from 1.0 × 10¹⁸cm^?3 to 2.8 × 10¹⁸ cm^?3 for which the effective mass was found to be equal to 0.55–0.76m₀. The Hall mobility, about 450cm²V^?1s^?1 at room temperature, obeys a $\text{T}{}^{\mathrm{<mtext>?3</mtext><mtext>2</mtext>}}$ law at high temperatures. On the basis of the electrical measurements the forbidden gap of Th₃As₄ was found to be equal to 0.43 eV.     

The average structure of 5.10-Dihydro-5.10-Diethylphenazinium-Iodide (E2P·I1.6): A new linear chain Polyiodide compound

Upon oxidation of 5.10-dihydro-5.10-diethylphenazine (E₂P) with iodine golden-green lustrous crystals of a compound with stoichiometry E₂P.I_1.6 were isolated. The compound crystallizes in the tetragonal space group D₄² with $\text{a = 12.321(2)}\text{A}\text{?}$ and $\text{c = 5.330(2)}\text{A}\text{?}$. The E₂P and I form interpenetrating incommensurate sublattices along c, with an iodine repeat distance of 9.7 Å. Static susceptibility measurements at room temperature give χ_g = + 0.994 × 10^?6g^?1 × cm³. This corresponds to one unpaired electron spin per two formular units. Single-crystal EPR indicates that the paramagnetism is associated with weakly interacting E₂P⁺ cation radicals. The 300K-d.c. conductivity of 3×10^?2Ω^?1cm^?1 and activation energy of 0.17±0.02eV for single crystals is consequently associated with the polyiodide chains, and not with the E₂P⁺ cation radicals.     

Electrical conductivity of pure and doped α-ferric oxides

Electrical conductivities of αFe₂O₃ containing 1 2, 2 3 and 3 8 mol% CdO were measured in the temperature range of 300 to 1300°C at Po₂'s of 10^?9 to 10^?1 atm Plots of log $\text{σ}\text{vs}\text{1}\text{T}$ at constant Po₂'s were found to be linear with an inflection at temperatures around 500°C and higher Po₂'s than 1 × 10^?4 atm. The activation energies obtained by the least-squares method were 1 34 eV for the intrinsic region and 0 51 eV for the extrinsic region on αFe₂O₃ doped with 38 mol% CdO The extrinsic conductivities disappeared at lower Po₂'s than 1 × 10^-4atm, and the intrinsic conduction appeared on the specimens investigated The electrical conductivities decreased with increasing amount of CdO doping The predominant defects in this system are believed to be interstitial Fe² for the intrinsic region and oxygen vacancies for the extrinsic region.     

Infrared optical properties of MoSe2

The infrared absorption spectrum of a single crystal of MoSe₂ is reported. A damped oscillator fit to the fundamental band gives the transverse optic frequency, $\text{Ω}{}_{\mathrm{TO}}\text{= 277}\text{cm}{}^{-1}$ at 300° K and $\text{Ω}{}_{\mathrm{TO}}\text{= 283}\text{cm}{}^{-1}$ at 77° K. The static and high frequency dielectric constants have been determined as K_s = 16.81 and K_∞ = 10.24 respectively. An absorption band appears in the i.r. spectrum at 482 cm^-1, and has been attributed to the oxygen impurity in the crystal.