层状的LiNi0.5Mn0.5O2合成及其电化学性能

采用超声波辅助溶胶-凝胶法合成层状的锂离子电池的正极材料LiNi0.5Mn0.5O2,并用热重分析、X射线衍射(XRD)、扫描电子显微镜(SEM)对材料的结构与形貌进行了研究,电化学性能采用循环伏安法(CV)、交流阻抗和充放电测试进行表征.结果表明,在950℃灼烧12 h的材料结晶度比较好,其晶胞参数a=0,287 9 nm,c=1.431 nm,结构比较理想.当材料在2.8～4.2 V间进行充放电时,其首次放电容量为170 mAh/g,50次循环后容量的保持率为89%.     

正交试验辅助分析溶胶-凝胶法制备Bi_(0.5)Na_(0.5)TiO_3粉体过程中的主导因素

以钛酸四丁酯、五水硝酸铋和无水乙酸钠为原料,用溶胶-凝胶法制备Bi0.5Na0.5TiO3(BNT)细粉,通过XRD和TEM表征粉体的结构和形貌。采用正交试验法,分析了反应温度、溶液pH值、加水量对最终BNT粉体粒径的影响。结果表明,各因素对粉体晶粒尺寸影响的显著性水平由大到小依次为加水量溶液pH值反应温度;反应温度为60℃、溶液pH值为4.5、加水量为7.2mL的条件下制得粉体的平均晶粒尺寸约为200～350nm。     

聚对苯撑/LiNi_（0.5）Fe_2O_4纳米复合热电材料的制备及其性能研究

本文以流变相反应法原位合成了聚对苯撑/LiNi_（0.5）Fe_2O_4纳米复合热电材料,并对其热电性能进行表征,研究了放电等离子烧结时保温时间对其热电性能的影响.结果发现,复合材料铁氧体颗粒粒径为100—300 nm,其外部被一层聚对苯撑膜包覆.电子在Fe~（2＋）和Fe~（3＋）之间的跳跃机理在铁氧体电导中占主导作用,因此聚对苯撑/LiNi_（0.5）Fe_2O_4复合材料具有n型导电特性.随着保温时间增加,复合材料电导率基本不变,但热导率逐渐增大且Seebeck系数逐渐减小,导致热电优值系数降低.由于结合了有机物高电导率和低热导率以及无机材料高赛贝克系数的优点,所制备的复合材料热电性能较单一材料有较大提高.     

HDDR工艺条件及均匀化处理对Nd12.6Fe69.3Co11.6 B6.0 Al0.5合金磁性能的影响

研究了HDDR工艺条件(包括HD温度、HD时间、DR温度、DR时间)对Nd12.6Fe69．3Co11.6B6．0Al0．5合金磁性能的影响；比较了均匀化处理和未均匀化处理的合金经HDDR工艺后磁性能的差异；通过对两种舍金原始态的XRD谱线分析，找出存在差异的原因。     

硅烷偶联剂表面处理对LiNi0.8Co0.15Al0.05O2结构和性能的影响

用硅烷偶联剂加热分解的简便方法对锂离子电池正极材料LiNi_0.8Co_0.15Al_0.05O₂(NCA)的表面进行处理, 利用XRD结合Rietveld精修、SEM、TEM、DSC、EIS和恒流充放电等方法对材料进行表征。结果显示, 硅烷偶联剂经450℃加热分解后得到的非晶态SiO₂均匀包覆在材料表面, 包覆不改变 NCA的晶体结构, 但明显改善了材料性能。在60℃环境中, 0.2C、1C下包覆材料(简写为a-NCA)的放电比容量分别为176.4、158.9 mAh·g^-1, 高于NCA的174.2、153.8 mAh·g^-1; 50周循环后a-NCA的容量保持率为91.4 %, 远高于NCA的86.5 %; 同时, 经包覆后材料的热稳定性大幅度提高。其原因是包覆层抑制了NCA在循环过程中与电解液发生副反应, 有效降低了离子迁移的界面膜电阻, 并抑制了晶体结构变化。     

电参数对Mg-7Gd-5Y-1.5Nd-0.5Zr镁合金微弧氧化膜的影响

针对Mg-7Gd-5Y-1.5Nd-0.5Zr高强耐热镁合金,采用微弧氧化工艺制备了表面防护层,研究了电流密度、电压、频率以及占空比等电参数对膜层厚度及形态的影响规律.研究表明,电压对氧化膜厚度影响显著,电流密度对氧化膜厚度有影响但不显著,占空比和频率对氧化膜厚度影响较小.随着电流及电压的增加,膜层表面微孔的尺寸逐渐增大;随频率和占空比的增加,膜层表面微孔的尺寸先增大后减小.     

Spinel LiNi0.5Mn1.5O4 cathode ion batteries： Nano vs micro,disordered phase （F4332） for rechargeable lithium- ordered phase （P433m）

Since the high-voltage spinel LiNi0.5Mn1504 （LNMO） is one of the most attractive cathode materials for lithium-ion batteries, how to improve the cycling and rate performance simultaneously has become a critical question. Nanosizing is a typical strategy to achieve high rate capability due to drastically shortened Li- ion diffusion distances. However, the high surface area of nanosized particles increases the side reaction with the electrolyte, which leads to poor cycling performance. Spinels with disordered structures could also lead to improved rate capability, but the cyclability is low due to the presence of Mn3＋ ions. Herein, we systematically investigated the synergic interaction between particle size and cation ordering. Our results indicated that a microsized disordered phase and a nanosized ordered phase of LNMO materials exhibited the best combination of high rate capability and cycling performance.     

Effect of annealing treatment on electrochemical property of LiNi0.5Mn1.5O4 spinel

LiNi0.5Mn1.5O4 was prepared under different cooling conditions. The electrochemical properties of LiNi0.5Mn1.5O4 prepared under different cooling conditions were investigated. The results show that LiNi0.5Mn1.5O4 synthesized with or without annealing treatment has similar X-ray diffraction patterns that can be indexed to cubic spinel structure. The mass loss occurring above 650℃ during the heating process can be mostly gained during the cooling process. LiNi0.5Mn1.5O4 synthesized with an annealing treatment exhibits almost one voltage plateau at around 4.7 V and higher capacity with a quick fading upon cycling, whereas LiNi0.5Mn1.5O4 synthesized without annealing treatment shows two voltage plateaus at around 4.1 and 4.7 V and superior capacity retention upon cycling both at rates of 1/7C and 1 C, though the capacity is not high.     

基于0.5μm CMOS工艺的高压器件

近年来,驱动类、音响类、接口类电路产品系列是CMOS集成电路发展的一个重要方向,这些电路中特有的高低压兼容结构是其重要的特点.相应地高低压兼容CMOS工艺技术应用也越来越广泛.本文研究了与常规CMOS工艺兼容的高压器件的结构与特性,在结构设计和工艺上做了大量的分析和实验,利用n-well和n管场注作漂移区,在没有增加任何工艺步骤的情况下,成功地将高压nMOS,pMOS器件嵌入在商用3.3/5V 0.5μm n-well CMOS工艺中.测试结果表明,高压大电流的nMOS管BVdssn达到23～25V,P管击穿BVdssp>19V.     

Improvement of microwave dielectric properties of the LiNb0.6Ti0.5O3 M-phase by doping with (Co1/3Nb2/3)4+

Structural evolution and microwave dielectric properties of LiNb_0.6(Ti_1-x[Co_1/3Nb_2/3]_x)_0.5O₃ (.05≤x≤.2) ceramics have been studied in this paper. Although the doped compositions maintain the M-phase solid solutions, compositional fluctuation due to nonuniform dispersion of minor dopants could be observed as x < .05, and trace amount of Li₂TiO₃-based solid solution (Li₂TiO₃ss) secondary phase presents in the x > .05 compositions. The microwave dielectric properties could be remarkably improved by the doping of (Co_1/2Nb_1/2)⁴⁺ in comparison to the undoped counterpart. Optimized microwave dielectric properties with Q × f = ∼6500 GHz, ε_r = ∼74 and τ_f = +8.2 ppm/°C could be obtained at x = .10 after sintering at 1050°C/2 h. The sintering temperature could be further reduced to 900°C/2 h by adding .2 wt% B₂O₃ without affecting significantly its microwave dielectric properties: ε_r = 73, Q × f = 6000 GHz, τ_f = +8.5 ppm/°C. The LiNb_0.6(Ti_1-x[Co_1/3Nb_2/3]_x)_0.5O₃ ceramics obtained in this case exhibit large dielectric permittivity coupled with much improved Q × f values, near zero τ_f, and low sintering temperature simultaneously, which makes it a promising high-k microwave dielectric material for low temperature cofired ceramic applications.