微波-固相复合加热技术合成LiNi0.5Co0.5O2及其性能研究

用高分子分散及微波-固相复合加热技术合成了层状锂离子电池正极材料LiNi0.5Co0.5O2. 采用循环伏安、充放电循环、扫描电子显微镜(SEM)以及X射线粉末衍射(XRD)等测试技术, 研究了煅烧条件对材料微观形貌、相结构以及电化学性能的影响规律. 研究结果表明: 在750 ℃煅烧4 h即可得到形状为类球形的纯相层状LiNi0.5Co0.5O2正极材料, 该材料的最大放电容量达到154 mA·h/g, 循环10周后放电容量仍保持在148 mA·h/g以上.     

聚苯胺/Co_(0.5)Zn_(0.5)Fe_2O_4纳米复合材料的制备及电磁性能

采用高分子凝胶法制备尖晶石型Co0.5Zn0.5Fe2O4,原位聚合法制备纯聚苯胺和聚苯胺/Co0.5Zn0.5-Fe2O4纳米复合材料.使用傅立叶红外光谱(FTIR)、紫外可见吸收光谱(UV-Vis)、X射线衍射仪(XRD)和透射电子显微镜(TEM)对复合材料进行了表征.FTIR和XRD的结果表明样品为纯聚苯胺和聚苯胺/Co0.5Zn0.5-Fe2O4.UV-Vis光谱表明聚苯胺/Co0.5Zn0.5Fe2O4苯环上的π-π*和n-π*分别红移了23nm和5nm.TEM照片可知,聚苯胺和聚苯胺/Co0.5Zn0.5Fe2O4粒子的平均粒径分别约为50nm和70nm.在8.2～12.4GHz测试频率范围内,聚苯胺/Co0.5Zn0.5Fe2O4的ε″数值在9.2～12.3之间,u″数值在0.15～0.16之间;聚苯胺/Co0.5-Zn0.5Fe2O4介电损耗低于纯聚苯胺,而磁损耗高于纯聚苯胺.     

PAni-Co0.5Zn0.5Nd0.05Fe1.95O4纳米复合材料的制备及电磁损耗

采用原位聚合法制备了平均粒径约为80 nm的聚苯胺(Polyaniline, PAni)-Co0.5Zn0.5Nd0.05Fe1.95O4纳米复合材料. 采用X射线衍射仪(XRD)、透射电子显微镜(TEM)和傅里叶变换红外光谱(FTIR)等检测技术对其结构、形貌、电磁及微波吸收性能进行了研究. 结果表明, 在12.4~18.0 GHz测试频率范围内, 复合材料的介电损耗角正切(tanε)在0.22~0.34之间, 磁损耗角正切(tanμ)在0.27~0.35之间. 在频率为9.5 GHz处, 反射损耗达到最大值-7.31×10-29 C·m, 频带宽为4.5 GHz.     

高倍率性能纳微结构锂离子电池正极材料0.6Li2MnO3-0.4LiNi0.5Mn0.5O2的简易制备

采用快速共沉淀法合成了立方体的层状无钴富锂固溶体正极材料0.6Li₂MnO₃-0.4LiNi_0.5Mn_0.5O₂.通过X射线衍射(XRD), X射线光电子能谱(XPS),电感耦合等离子体(ICP),扫描电子显微镜(SEM),透射电子显微镜(TEM)及电性能测试等手段对材料进行了表征.结果表明,材料具有典型的α-NaFeO₂六方层状晶体结构且具有与目标材料相似的化学组成. SEM和TEM结果表明,材料由粒径为40-200 nm的纳米颗粒组装成立方体结构.在文中给出了一个立方团聚体可能的形成机理.电化学性能测试(2.0-4.8 V电压范围内(vs Li/Li⁺))显示该材料具有优异的倍率性能, 0.1C和10C倍率下的放电比容量分别是243和143 mAh·g^-1.此外,该材料具有良好的循环稳定性,即使在大倍率测试后, 0.5C倍率下循环72次仍显示出90.7%的高容量保持率.这种具有简易操作步骤和优异结果的共沉淀方法是一种经济的能够促进锂离子电池正极材料大规模应用的技术手段.     

Sm0.5Sr0.5Co1-xCuxO3-δ阴极材料的合成与性能研究

采用尿素-硝酸盐法制备了Sm0.5Sr0.5Co1-xCuxO3-δ(x=0～0.5)阴极材料.用TG-DSC,SEM,XRD和热膨胀仪对材料的形成过程、晶体结构、烧结体的微观结构及热膨胀性能进行了表征.用直流四端子法测试材料在500～800℃范围内的电导率.结果表明,制备样品的主晶相为正交钙钛矿结构,体系含有杂相;电导率随温度和Cu含量的变化关系表现为,x≤0.2时的样品随温度升高电导率降低,x≥0.3时随温度升高电导率增大,组成为x=0.2的样品电导率最高,500℃达到703.1 S·cm-1.材料的热膨胀系数随掺杂的Cu含量增加而降低.     

Na0.5La0.5TiO3的水热法合成及其表征

通过控制反应物摩尔比、晶化温度和时间以及体系的碱度等重要因素,用水热法在温和的条件下合成了Na0.5La0.5TiO3;结构分析表明单相的Na0.5La0.5TiO3是具有立方对称性的钙钛矿型化合物,晶胞参数为3.875(。A);初步认为该化合物合成过程为溶解-沉淀机理.     

B掺杂Cd0.5Zn0.5S光催化剂制氢性能研究

采用浸渍法制备了B掺杂的Cd0.5Zn0.5S光催化剂,考察了不同B掺杂量的Cd0.5Zn0.5S催化剂在可见光光照下的放氢活性和稳定性.实验结果表明,B掺杂可以显著提高催化剂的活性和稳定性.B的掺杂量对催化剂的活性有显著影响,最佳担载量为2%.在利用XRD、PL、XPS、UV-V is等手段对催化剂表征的基础上,结合光催化性能测定结果与催化剂表征结果,初步探讨了B掺杂对Cd0.5Zn0.5S光催化剂性能的影响机制.结果表明,B掺杂显著地增强了B/Cd0.5Zn0.5S催化剂的紫外-可见漫反射和荧光光谱强度.XPS结果表明,催化剂中的B物种不是以简单氧化物的形式存在,而可能是通过某种化学反应与Cd0.5Zn0.5S光催化剂作用,使催化剂的性能得以改善.     

不同组分下富锂正极材料xLi_2MnO_3·(1-x)LiNi_(0.5)Mn_(0.5)O_2(x=0.1-0.8)的晶体结构与电化学性能

采用溶胶-凝胶法制备了一系列富锂锰基正极材料xLi2MnO3?(1-x)LiNi0.5Mn0.5O2(x=0.1-0.8),通过X射线衍射(XRD)仪,扫描电子显微镜(SEM)和电化学测试等检测手段表征了所得样品的晶体结构与电化学性能,研究了不同组分下富锂材料的结构与电化学性能.结果表明:Li2MnO3组分含量较高时,材料的首次放电容量较高,但循环稳定性较差;该组分含量较少时,所得样品中出现尖晶石杂相,且放电容量较低,但循环稳定性较好;综合来看,x=0.5时材料的电化学性能最优.x=0.4,0.6时材料也表现出了较好的电化学性能,值得关注.     

BaCe0.5Zr0.4Y0.1O3-δ粉体的溶胶-凝胶法和高温固相法制备及性能表征

分别通过溶胶-凝胶法和高温固相反应法制备了BaCe0.5Zr0.4Y0.1O3-δ粉体.采用热重-差热分析(TG-DTA),粉末X射线衍射(XRD),扫描电子显微镜(SEM),傅立叶红外衍射(FT-IR),N2吸附-脱附等方法对所制备的粉体进行了表征.结果表明:用溶胶-凝胶法在1200 ℃×10 h可以合成纯的BaCe0.5Zr0.4Y0.1O3-δ粉体,合成温度比传统的高温固相反应法降低400 ℃左右;溶胶-凝胶法合成粉体具有多孔结构特征,与固相法合成粉体相比具有较高的比表面积.但致密化试验表明:溶胶-凝胶法合成粉体与固相法合成粉体相比具有较低的烧结活性.溶胶-凝胶法合成粉体颗粒表面残余的有机基团和颗粒内部的大量微孔将在致密化过程中产生空间位阻,从而影响高温下原子的迁移,阻碍材料的致密化过程.     

正极材料LiNi0.5Co0.5O2的电化学性能研究

以聚丙烯酰胺(PAM)为分散剂用微波—固相复合加热技术合成了层状锂离子电池正极材料LiNi0.5Co0.5O2。通过扫描电子显微镜(SEM)和X—射线粉末衍射(XRD)分析技术对材料的微观形貌和相结构进行了表征。恒电流充放电循环测试表明:材料的放电比容量高达154mAh/g,且有良好的循环性能。重点利用循环扫描伏安、计时电量和电化学交流阻抗测试技术,对材料在循环前后的电化学性能变化规律进行了探讨。结果表明,经过循环后材料的导电能力以及锂离子扩散能力都有了很大的提高。另外,材料中的锂含量对材料的导电能力也有很大的影响。     

Hydrothermal Synthesis of Pb_(1-1.5x)La_xZr_(0.5)Ti_(0.5)O_3 (x = 0.01-0.06) Nanocrystallites

Lanthanum doped lead zirconate titanate (PLZT) ceramics display excellent electrooptic and photostriction properties because of the existence of cavities in the perovskite structure1-3. The PLZT powders are conventionally prepared by solid state reaction4-5, and the wet chemical methods such as sol-gel techniques are then introduced6-7. However, the homogeneity, morphology and size of the particles, which greatly affect the sinterability and the property of the resulting ceramics, are dif…     

Phase separation and superconductivity in Fe(1+x)Te(0.5)Se(0.5)

Fe(1+x)Te(0.5)Se(0.5) is the archetypical iron-based superconductor. Here we show that the superconducting state is controlled by the stacking of its anti-PbO layers, such that homogeneous ordering hinders superconductivity and the highest volume fractions are observed in phase separated structures as evidenced by either a distribution of lattice parameters or microstrain.     

Theoretical probing of deltahedral closo-auroboranes B(x)Au(x)2- (x = 5-12)

Using density functional theory calculations, here we show that a series of B(x)Au(x)2- (x = 5-12) dianions possesses structure and bonding similar to the famous deltahedral closo-borane cages, B(x)H(x)2-. Effective atomic charges on Au in B(x)Au(x)2- are very similar to those on H in B(x)H(x)2-, indicating that Au in the closo-auroboranes is indeed analogous to H in the closo-boranes. The present theoretical predictions of B(x)Au(x)2- suggest that the closo-auroborane species are viable new chemical building blocks that may be synthesized in bulk. The Au atoms in the closo-auroboranes represent highly atomically dispersed Au and may potentially exhibit novel catalytic and chemical properties.     

BaCe1—xRExO3—0.5x的溶胶—凝胶法合成及离子导电性

用溶胶－凝胶法合成了系列钙钛矿结构的ＢａＣｅ１－ｘＲＥｘＯ３－０．５ｘ（ＲＥ＝Ｌａ，Ｎｄ，Ｓｍ，Ｅｕ，Ｇｄ，Ｄｙ，Ｈｏ，Ｅｒ和Ｙ）复合氧化物，通过ＸＲＤ和热分析对样品结构及生成过程进行了研究．测定了不同温度下样品的交流阻抗谱，讨论了稀土离子掺杂对ＢａＣｅＯ３电性质的影响．溶胶－凝胶法比固相反应法合成温度降低了６００～８００℃，稀土掺杂使ＢａＣｅＯ３离子导电率提高了１０～４０倍．     

La10(SiO4)6－x(GaO4)xO3－0.5x的合成及其导电性能

以溶胶-凝胶法合成前驱体, 在950 ℃时烧结制得La10(SiO4)6－x(GaO4)xO3－0.5x (x＝0, 0.5, 1.0, 1.5和2.0)陶瓷样品, 通过TG-DTA, XRD, IR和SEM表征, 所得产品为磷灰石相. 以电化学阻抗谱研究了其导电性能, 发现决定电导率大小的因素有两种, 一是间隙氧的数量, 二是晶胞的大小, 两种因素的综合作用, 使得La10(SiO4)5(GaO4)O2.5的电导率最大, 在700 ℃时其电导率达到4.66×10－2 S•cm－1. 离子迁移数和氧分压对电导率的研究表明, 其主要的电荷载体是O2－离子.     

Phase evolution, phase transition, raman spectra, infrared spectra, and microwave dielectric properties of low temperature firing (K(0.5x)Bi(1-0.5x))(Mo(x)V(1-x))O4 ceramics with scheelite related structure

In the present work, the (K(0.5x)Bi(1-0.5x))(Mo(x)V(1-x))O(4) ceramics (0≤x ≤ 1.00) were prepared via the solid state reaction method and sintered at temperatures below 830 °C. At room temperature, the BiVO(4) scheelite monoclinic solid solution was formed in ceramic samples with x < 0.10. When x lies between 0.1-0.19, a BiVO(4) scheelite tetragonal phase was formed. The phase transition from scheelite monoclinic to scheelite tetragonal phase is a continuous, second order ferroelastic transition. High temperature X-ray diffraction results showed that this phase transition can also be induced at high temperatures about 62 °C for x = 0.09 sample, and has a monoclinic phase at room temperature. Two scheelite tetragonal phases, one being a BiVO(4) type and the other phase is a (K,Bi)(1/2)MoO(4) type, coexist in the compositional range 0.19 < x < 0.82. A pure (K,Bi)(1/2)MoO(4) tetragonal type solid solution can be obtained in the range 0.82 ≤ x ≤ 0.85. Between 0.88 ≤ x ≤ 1.0, a (K,Bi)(1/2)MoO(4) monoclinic solid solution region was observed. Excellent microwave dielectric performance with a relative dielectric permittivity around 78 and Qf value above 7800 GHz were achieved in ceramic samples near the ferroelastic phase boundary (at x = 0.09 and 0.10).     

A facile approach to synthesize high-quality Zn(x)Cu(y)InS(1.5+x+0.5y) nanocrystal emitters

A facile approach to synthesize Zn(x)Cu(y)InS(1.5+x+0.5y) nanocrystal emitters was presented. The compositions of these nanocrystals were precisely controlled, and the relative PL quantum yields were up to 40%, with tunable emissions in 450-640 nm.     

Crystallographic and electrochemical characteristics of La(0.7)Mg(0.3)Ni(5.0-x)(Al(0.5)Mo(0.5)x hydrogen-storage alloys.

The structure, hydrogen-storage property and electrochemical characteristics of La(0.7)Mg(0.3)Ni(5.0-x)(Al(0.5)Mo(0.5))x (x = 0-0.8) hydrogen-storage alloys have been studied systematically. X-ray diffraction Rietveld analysis shows that all the alloys consist of an La (La,Mg)2Ni9 phase and an LaNi5 phase. The pressure-composition isotherms indicate that the hydrogen-storage capacity first increases and then decreases with increasing x, and the equilibrium pressure decreases with increasing x. Electrochemical measurements show that the maximum discharge capacity and the exchange-current density of the alloy electrodes increase as x increases from 0 to 0.6 and then decrease when x increases further from 0.6 to 0.8. Moreover, the low-temperature dischargeability of the alloy electrodes increases monotonically with increasing x in the alloys.     

Local electronic structure of layered Li(x)Ni0.5Mn0.5O2 and Li(x)Ni(1/3)Mn(1/3)Co(1/3)O2

Samples of Li(x)Ni0.5Mn0.5O2 and Li(x)Ni(1/3)Mn(1/3)Co(1/3)O2 were prepared as active materials in electrochemical half-cells and were cycled electrochemically to obtain different values of Li concentration, x. Absorption edges of Ni, Mn, Co, and O in these materials of differing x were measured by electron energy loss spectrometry (EELS) in a transmission electron microscope to determine the changes in local electronic structure caused by delithiation. The work was supported by electronic structure calculations with the VASP pseudopotential package, the full-potential linear augmented plane wave code WIEN2K, and atomic multiplet calculations that took account of the electronic effects from local octahedral symmetry. A valence change from Ni2+ to Ni4+ with delithiation would have caused a 3 eV shift in energy of the intense white line at the Ni L3 edge, but the measured shift was less than 1.2 eV. The intensities of the "white lines" at the Ni L-edges did not change enough to account for a substantial change of Ni valence. No changes were detectable at the Mn and Co L-edges after delithiation either. Both EELS and the computational efforts showed that most of the charge compensation for Li+ takes place at hybridized O 2p states, not at Ni atoms.