高分子自组装Mn2O3花瓣状纳米带、纳米线的研究

通过控制热处理工艺条件, 利用Mn(CH3COO)2和具有特殊空间构型的聚乙烯醇(PVA), 在600 ℃合成了类花瓣状Mn2O3纳米带和纳米线结构. SEM, XRD表征分析证明Mn2O3纳米带结构为方铁锰矿晶型结构, 沿(222)方向择优生长. 分析了热处理工艺对一维纳米结构的影响机制. 初步探讨了Mn2O3一维纳米结构的生长机理.     

Mn3O4多面体纳米晶体的制备及其电化学性能

通过对未加添加剂的醋酸锰-乙醇体系的一种简易的水基热解过程,制备了Mn3O4多面体纳米晶体。借助X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、傅里叶变换红外光谱法(FTIR)、拉曼光谱和X-射线光电子能谱(XPS)等对Mn3O4的结构和形貌进行了表征。提出了Mn3O4多面体纳米晶体的形成机理。循环伏安法(CV)测试结果表明,所制得的Mn3O4电极呈现良好的赝电容性能。在扫描速率为5 mV.s-1时,得到了Mn3O4的最大比电容值173 F.g-1。     

Gd3Ga5O12∶Eu3+发光纳米晶的燃烧合成及性质

以尿素为燃烧剂,乙二醇为分散剂采用燃烧法制备了Gd3Ga5O12∶Eu3+纳米晶。利用X射线衍射、电镜和荧光光谱对前驱体和热处理后样品的结构、形貌和发光性能进行了表征。XRD结果表明:700℃热处理2 h即可获得立方结构Gd3Ga5O12∶Eu3+纳米晶。根据Scherrer公式估算经700℃和900℃热处理2 h获得的纳米晶的一次性粒径分别为28 nm和42 nm。发射光谱和激发光谱的结果表明:特征发射峰来自于5D0-7FJ跃迁,而来自于Eu3+的5D0→7F1的磁偶极跃迁发射最强;宽激发带主要来自于Eu-O电荷迁移带和Gd3Ga5O12基质吸收。发射强度和激发强度随热处理温度的提高而增强。     

一维ZnO表面可控构建Co3Mn1纳米晶及其催化CO氧化性能

利用热分解法制备了结构明确的负载型纳米晶催化剂。在纳米晶成核和生长过程中加入一维Zn O纳米棒作为晶种,调控不同组分的纳米晶在Zn O纳米棒表面均匀生长,从而获得了结构明确的Mn O/Zn O、Co₃O₄/Zn O、Co₃Mn₁/Zn O催化剂。透射电子显微镜(TEM)与X射线粉末衍射(XRD)结果显示,不同组分纳米颗粒都均匀分散在Zn O纳米棒表面。相对于Mn O/Zn O和Co₃O₄/Zn O催化剂,Co₃Mn₁/Zn O催化剂在CO氧化反应中具有最佳的催化性能。在200 L·g^-1_cat·h^-1的气时空速下,Co₃Mn₁/Zn O催化剂起活温度为50℃,其T₁₀₀(CO转化率达到100%时的温度)为200℃;利用X射线光电子能谱(XPS)对不同催化剂进行了分析,结果显示,Co<...     

锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2的制备及其电化学性能

以Ni1/3Co1/3Mn1/3(OH)2(2)和Li2CO3为原料,在空气气氛中,经过高温热处理工艺制备了高结晶度的锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2(1)。正交试验确定最佳工艺条件为:2 0.3 mol,n(Li):n(2)=1.2,于950℃反应13 h。电化学性能研究结果表明,在2.7 V～4.6 V,电流密度16 mA.g-1时,1的首次放电比容量为203.4 mAh.g-1;经16 mA.g-1循环2次,32 mA.g-1循环9次,80 mA.g-1循环20次后放电比容量为164.1 mAh.g-1。     

锂离子电池用α-Fe2O3-Ag复合纳米棒负极材料的制备及储锂性能

采用FeOOH纳米棒为前驱体,通过层层自组装法及随后的热处理过程制备出α-Fe2O3-Ag复合纳米棒.采用透射电子显微镜(TEM)、高分辨透射电子显微镜(HRTEM)和电化学性能测试对样品的形貌、结构及电化学性能进行了表征.结果表明,Ag纳米颗粒均匀地分布在α-Fe2O3纳米棒的表面.作为锂离子电池负极材料,α-Fe2O3-Ag复合纳米棒表现出了较好的循环性能和较高的比容量.180个循环后,其比容量高达549.8 mA.h/g.     

锂离子电池镍掺杂尖晶石LiMn2O4正极材料的电子结构

采用密度泛甬平面波赝势方法对LiMn2O4和LiNi0.5Mn1.5O4的几何结构进行了优化,并计算了相应的电子结构.计算的结果表明:在Li 脱嵌前后,LiMn2O4和LiNi0.5Mn1.5O4均为导体,且锂元素主要以离子形式存在于两种材料中,O2p轨道与Mn(Ni)的3d轨道形成了较强的共价键.Li 嵌入导致Mn(Ni)3d轨道的态密度峰发生移动.Ni的掺杂导致Mn(Ni)和O2p轨道的成键作用得以加强,电子在Mn(Ni)3d轨道的填充发生变化,从而提高了电池的充放电电压.     

水热法合成ReMn2O5(Re=Gd，Sm，Yb)纳米粉体

本文采用水热法,以KMnO4和Mn(C2H3O2):为锰源,在250℃反应24 h合成了高各向异性的GdMn2O5、SmMn2O5和YbMn2O5纳米粉体.利用X射线粉末衍射(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、选区电子衍射(SAED)、和高分辨透射电镜(HRTEM)对产物的结构和形貌进行了表征.结果表明,所制备的ReMn2O5(Re=Gd,Sm,Yb)均为正交相结构.反应溶液中碱性矿化剂浓度对产物的形貌和尺寸有重要的影响.通过实验结果分析了纳米结构的形成机理.     

无机-有机杂化硫属化合物[Mn(1,2-dap)2(H2O)]2(μ-Sn2Q6)(Q=S、Se)和[Mn(tren)]2(μ-Sn2S6)的合成、晶体 结构与性能

采用溶剂热方法合成了3个多元硫属化合物[Mn(1,2-dap)2(H2O)]2(μ-Sn2Q6)(Q=S(1)和Se(2))和[Mn(tren)]2(μ-Sn2S6)(3),用X-射线单晶衍射测定了化合物的结构,并通过红外光谱、紫外-可见漫反射光谱对其进行了表征。单晶结构解析表明,化合物1和2都属于正交晶系,Pccn空间群(No.56),晶体结构是由[Mn(1,2-dap)2(H2O)]2+配合物阳离子和[Sn2Q6]4-二聚体通过Mn-Q键连接而成的[Mn(1,2-dap)2(H2O)]2(μ-Sn2Q6)低聚体,相邻的低聚体之间通过氢键相连形成三维结构。化合物3属于三斜晶系,晶体结构是由[Mn(tren)]2(μ-Sn2S6)单元通过氢键连接而成的二维结构。紫外-可见漫反射光谱结果显示化合物1,2和3的带隙分别为2.5,2.1,2.4 e V,属于半导体材料。     

静电纺丝法制备V2O5微纳米棒及光催化性能

以聚乙烯吡咯烷酮(PVP)和偏钒酸铵(NH4VO3)为原料,利用静电纺丝技术结合溶胶过程制备PVP/NH4VO3纤维,对纤维缓慢控温处理制备V2O5微纳米棒。采用热重-差热分析(TG-DTA)、X射线衍射光谱(XRD)、傅立叶红外光谱(FT-IR)、场发射扫描电子显微镜(FE-SEM)、X射线光电子能谱(XPS)和紫外-可见漫反射光谱(UV-Vis)技术手段对V2O5微纳米棒的结构和表面形态进行表征。以亚甲基蓝(MB)的光降解为模型反应,研究V2O5微纳米棒的光催化性能。结果表明:热处理温度对催化剂表面形态和晶相的生长有明显影响,550℃煅烧的V2O5微纳米棒在可见光区对MB的光降解效率最高,并分析和探讨了可能的光催化机理。     

Uniform MgO nanobelts formed from in situ Mg3N2 precursor

MgO nanobelts with a pure morphology and high yield were generated by the direct evaporation of Mg metals under initial N₂ gas at 650 °C and subsequent N₂/O₂ atmosphere at 800 °C. The growth of these MgO nanobelts is explained in a VS route in which the in situ formed Mg₃N₂ slowly decomposes and reacts with oxygen. Mg₃N₂ is therefore a very effective precursor for the fabrication of high-purity one-dimensional (1D) MgO nanostructures.     

Mn2O3纳米结构的简易合成与电化学性质

用简易的室温或水热方法制备出不同形貌的MnCO₃微结构。经600 ℃热处理后,室温制备MnCO₃转变成Mn₂O₃胶体片,而水热制备MnCO₃样品则形成多孔Mn₂O₃纳米结构。然而,室温制备MnCO₃经120 ℃热处理后形成Mn₂O₃晶相。制备样品经过XRD和SEM表征表明,热处理MnCO₃前驱物形成Mn₂O₃过程导致产物形貌与结构变化。其形成机理又通过TEM和FTIR进一步研究。Mn₂O₃纳米结构的电容性质通过循环伏安法表征,结果表明Mn₂O₃形貌与结构对其电容有重要影响。     

Y2O3包覆LiCo1/3Ni1/3Mn1/3O2的电化学性能

通过在硝酸钇水溶液浸渍并焙烧的简单工艺, 在LiCo1/3Ni1/3Mn1/3O2材料表面包覆了一层Y2O3. 采用X射线衍射(XRD), 扫描电子显微镜(SEM), 透射电子显微镜(TEM), 循环伏安(CV)和恒流充放电对包覆和未包覆的LiCo1/3Ni1/3Mn1/3O2进行了测试分析. 结果表明, Y2O3包覆并没有改变LiCo1/3Ni1/3Mn1/3O2的晶体结构, 只存在于LiCo1/3Ni1/3Mn1/3O2的表面; 与未包覆的材料相比, Y2O3包覆后的材料在高电位下具有更好的容量保持率和放电容量. CV测试表明, 包覆层的存在有效抑制了材料层状结构的转变及电极与电解液的负反应.     

TiO2包覆对LiCo1/3Ni1/3Mn1/3O2材料的表面改性

为了提高材料LiCo1/3Ni1/3Mn1/3O2的循环性能, 采用浸渍-水解法对其进行TiO2包覆. 用X射线衍射(XRD)、电化学交流阻抗谱(EIS)、电感耦合等离子体发射光谱(ICP-OES)和恒流充放电测试研究包覆材料的结构和电化学性能. TiO2仅在材料表面形成包覆层, 并未改变材料的结构. TiO2包覆能提高材料LiCo1/3Ni1/3Mn1/3O2的倍率性能和循环性能, TiO2包覆后的材料在5.0C(1.0C=160 mA·g-1)下的放电容量达到0.2C下的66.0%, 而包覆前的材料在5.0C下的放电容量仅为其0.2C下的31.5%. 包覆后的材料在2.0C下循环12周后的容量没有衰减, 而未包覆的材料容量保持率仅为94.4%. EIS测试表明包覆材料性能的提高是由于循环过程中材料的界面稳定性得到了提高. 循环后材料的XRD和ICP-OES测试表明, 包覆层能提高材料LiCo1/3Ni1/3Mn1/3O2的结构稳定性.     

锌掺杂提高LiNi1/3Co1/3Mn1/3O2正极材料的电化学稳定性

通过共沉淀法与固相法相结合制备了掺锌的高稳定性Li(Ni_1/3Co_1/3Mn_1/3)_1-xZn_xO₂ (x=0, 0.02, 0.05)正极材料. 循环伏安(CV)曲线表明Zn掺杂使氧化峰与还原峰的电势差减小到0.09 V, 电化学阻抗谱(EIS)曲线表明Zn掺杂使电极的阻抗从266 Ω减小到102 Ω. Li⁺嵌入扩散系数从1.20×10^-11 cm²·s^-1增大到 2.54×10^-11 cm²·s^-1. Li(Ni_1/3Co_1/3Mn_1/3)_0.98Zn_0.02O₂正极材料以0.3C充放电在较高的截止电压(4.6 V)下比其他两种材料的电化学循环性能更稳定, 其第二周的放电比容量为176.2 mAh·g^-1, 循环100周后容量几乎没衰减; 高温(55 °C)下充放电循环100周, 其放电比容量平均每周仅衰减0.20%, 远小于其他两种正极材料(LiNi_1/3Co_1/3Mn_1/3O₂平均每周衰减0.54%; Li(Ni_1/3Co_1/3Mn_1/3)_0.95Zn_0.05O₂平均每周衰减0.38%). Li(Ni_1/3Co_1/3Mn_1/3)_0.98Zn_0.02O₂正极材料以3C充放电时其放电比容量可达142 mAh·g^-1, 高于其他两种正极材料. 电化学稳定性的提高归因于Zn掺杂后减小了电极的极化和阻抗, 增大了锂离子扩散系数.     

Li2CO3、NiO和电解MnO2合成高容量LiNi0.5Mn1.5O4及其表征

Well-developed crystalline LiNi_0.5Mn_1.5O₄ was prepared by solid-state reaction using Li₂CO₃, NiO and electrolytic MnO₂ at high heating and cooling rate. X-ray diffraction (XRD) patterns and scanning electron microscopic (SEM) images showed that LiNi_0.5Mn_1.5O₄ synthesized at 900 ℃ and 950 ℃ had cubic spinel structure with clearly defined shape. LiNi_0.5Mn_1.5O₄ spinel phase decomposed at 1 000 ℃ accompanying with structural and morphological degradation. TG measurement revealed that the weight loss during heating process could be mostly gained in cooling process, and the upward tendency of weight loss during heating process decreased, while that of irreversible weight loss rapidly increased with the increase of temperature. LiNi_0.5Mn_1.5O₄ powders prepared at 900 ℃ for 12 h delivered the maximum discharge capacity of 134 mAh·g^-1 with good cyclic performance at 2/7 C. In addition, by adjusting the calcination time at 900 ℃, the capacity and cycling performance of LiNi_0.5Mn_1.5O₄ were further enhanced.     

负载型La0.8Sr0.2MnO3燃烧催化剂的载体效应

Combustion catalysts La0.8Sr0.2MnO3 supported on γ-Al2O3, α-Al2O3, cordierite (2MgO•2Al2O3•5SiO2) and ZrO2 were compared. Further investigation was focused on LSM/ γ-Al2O3 catalyst. It was observed that LSM/γ－Al2O3 catalyst loaded with 20% (mass fraction) LSM (La0.8Sr0.2MnO3 or corresponding oxides), heated at 750℃ or above, perovskite-type oxides were found by XRD examination, whereas, the same catalyst loaded with 10% or less LSM, perovskite oxides were absent, calcination temperature about 750℃ is necessary for the formation of perovskite structure in LSM/γ-Al2O3 catalysts. High activity of complete oxidation of xylen will be obtained when perovskite-type oxides.
Investigation of TPR showed that neat LSM or LSM/γ-Al2O3(20%) was reduced by H2-N2 mixed gas. Two degradation processes took place. In the first, reduced temperature peak was about 350 - 450℃. If reduction ended at 400℃, perovskite structure was retained, which may be due to the reduction of Mn3+to Mn2+ on the surface of LSM only. In the second process, perovskite structure was destroied, and La2O3, Mn2O3, Mn - Sr - O oxides could be obtained, which took place in the temperature range 685 - 750℃ and ended at 800℃. This was proved by TPR experiments (Fig. 3, 5) and XRD patterns (Fig. 4)
Catalysts LSM/γ-Al2O3(10% or 20%) heated at 500℃ have only one TPR peak, i. e. lower temperature peak. This is due to the absence of perovskite-type oxides in the catalysts. However, neat LSM or LSM/γ-Al2O3(20%) heated 750℃ or above, not only the first low temperature TPR peak but also the second peak, which is contributed by the perovskite-type oxides in these catalysts appeared. Therefore, the second TPR peak, i. e. the higher temperatue peak is a characteristic peak for perovskite-type oxides in the reduced process. When LSM/ γ-Al2O3 (10%) catalys is heated at 750℃, no perovskite-type oxides were detected by XRD, and the second reduction peak was absent also in TPR process. \
The order of the second reduction peak temperature(characteristic peak of perovskite - type ox- ides) is: neat LSM(750℃）> LSM/γ-Al2O3 20% (685-698℃) -deposited LSM/γ-Al2O3 (698℃) > LSM/γ-Al2O3 15% (677 - 680℃) >(LSM/γ-AL2O3 10% 620 - 630℃, for Mn - Al - O medium oxides on surface). It is correleted with the increasing of the effect of support sequentially.
When LSM/γ-Al2O3 catalysts were heated at 900℃, more stable phase, spinel MnAl2O4 appeared, which could be proved by TPR of model catalyst MnAl2O4/γ-Al2O3.     

Water oxidation electrocatalyzed by an efficient Mn3O4/CoSe2 nanocomposite

The design of efficient, cheap, and abundant oxygen evolution reaction (OER) catalysts is crucial to the development of sustainable energy sources for powering fuel cells. We describe here a novel Mn(3)O(4)/CoSe(2) hybrid which could be a promising candidate for such electrocatalysts. Possibly due to the synergetic chemical coupling effects between Mn(3)O(4) and CoSe(2), the constructed hybrid displayed superior OER catalytic performance relative to its parent CoSe(2)/DETA nanobelts. Notably, such earth-abundant cobalt (Co)-based catalyst afforded a current density of 10 mA cm(-2) at a small overpotential of ~0.45 V and a small Tafel slope down to 49 mV/decade, comparable to the best performance of the well-investigated cobalt oxides. Moreover, this Mn(3)O(4)/CoSe(2) hybrid shows good stability in 0.1 M KOH electrolyte, which is highly required to a promising OER electrocatalyst.     

六方相WO3纳米带的制备与表征

以Na2WO4、K2SO4和H2C2O4为原料,采用两步水热合成法制备了六方相WO3纳米带.首先,在探索pH值、K2SO4加入量、反应温度和时间以及表面活性剂等因素对WO3纳米带的前驱物钨酸盐形貌的影响后,给出了前驱物钨酸盐纳米带的合成条件,并讨论了纳米带的形成机理;然后,在180℃的水热条件下对前驱物再处理48 h获得六方相WO3纳米带.测试结果表明,WO3纳米带的形貌保持较好,宽度在100～300 nm间,长度可达数微米,沿纳米带长轴方向为[001]方向.     

氧化铟八面体、纳米带、锯齿状纳米线和纳米链的可控合成

在N₂/H₂O混合气流中将硅片上金覆盖的金属铟颗粒加热到800 ℃制备出了不同形貌的In₂O₃纳米结构, 在距铟源不同距离处依次得到In₂O₃的八面体、纳米带、锯齿状纳米线和纳米链. 采用拉曼光谱、扫描电镜、X射线衍射和透射电镜对产物进行了表征分析. 结果表明, 八面体、纳米带、锯齿状纳米线和纳米链均为立方相单晶结构的In₂O₃. 基于气-固和气-液-固生长机理详细分析了八面体、纳米带、锯齿状纳米线和纳米链的生长过程, 提出了不同形貌In₂O₃纳米结构的生长模式.