熔融浸渍法合成单晶锰酸锂作为锂离子电池阴极材料

以二氧化锰和氢氧化锂为原料,通过熔融浸渍法合成具有尖晶石构型的单晶锰酸锂。前驱体β-MnO₂以乙酸锰和过硫酸钠为原料通过水热反应合成。基于TGA/DTA测试,确定了单晶锰酸锂的煅烧温度为470℃预烧5h,再升温至750℃保温12h。XRD,FTIR和SEM结果表明,合成的单晶锰酸锂具有均一的棒状结构以及良好的结晶性。电化学性能测试结果表明材料在0.1C倍率下充放电时,其首次放电比容量可达126mAh·g^-1,且在一百次循环之后容量保持率为91%。     

稻壳基活性炭对锰酸锂电池倍率性能的影响

稻壳基活性炭(RH-AC)具有天然的多级孔道结构,是由稻壳碳化和活化两步得到的。 用RH-AC和锰酸锂(LMO)混合制备复合电极,以锂片为对电极,组装半电池进行恒流充放电测试。 实验发现:含有质量分数为5%的RH-AC与90.5%的LMO的复合电极(RH-AC5)在5C电流密度循环100圈后比容量为89.3 mA·h/g,容量保持率高于89%,远优于纯锰酸锂电极。 采用循环伏安法计算出的锂离子扩散系数,及利用交流阻抗测试拟合后得到的结果进一步验证了该结论。     

正硅酸乙酯对高电压镍锰酸锂基全电池电化学性能的影响

为了提高镍锰酸锂全电池的电化学性能,本文采用物理混合的方法在负极浆料中加入正硅酸乙酯(TEOS),并按m(TEOS)∶m(石墨)=0∶100、5∶100、10∶100、16∶100、20∶100的比例进行搅拌混合。 以镍锰酸锂为正极,石墨为负极,组装成502030型软包装锂离子电池,并对该电池进行恒流充放电和内阻等测试。 测试结果显示,0TEOS(m(TEOS)∶m(石墨)=0∶100)样品的电池内阻为159 mΩ,循环200圈后,容量保持率为52.6%,放电比容量为46 mA·h/g;16TEOS(m(TEOS)∶m(石墨)=16∶100)样品的电池为105 mΩ,65.7%和62.9 mA·h/g。 实验结果表明:通过物理混合的方法在负极浆料中加入TEOS,有利于在负极表面形成结构稳定的人工固体电解质膜(SEI膜),提高镍锰酸锂材料的循环和倍率性能。     

单斜层状结构锂离子电池正极材料LiYxMn1-xO2的合成及电化学性能

以Na2CO3 、(CH3CO2)2Mn•4H2O、Y2O3和CH3COOLi•2H2O为原料,采用高温固相法经过2次灼烧和水热离子交换法得到一系列钇掺杂的LiMn1-xYxO2 (x=0.01,0.02,0.03,0.05) 化合物。通过XRD、XPS、循环伏安及恒电流充放电测试,研究了钇掺杂离子对合成正极材料结构及电化学性能的影响。X射线衍射测试结果表明,所得产物均具有单斜层状结构。循环伏安及恒电流充放电测试结果表明,合适的钇掺杂可以起到扩展锂离子脱嵌通道和稳定骨架结构的作用, 钇离子的引入可以部分取代原有的三价锰离子, 由于钇离子的离子半径较三价锰离子大, 因此稀土掺杂锰酸锂材料的晶胞参数比未掺杂材料大, 在一定程度上扩充了锂离子迁移的三维通道, 更有利于锂离子的嵌入与脱嵌,提高单斜层状LiMnO2 材料的电化学循环可逆性及循环稳定性。通过对所得化合物进行了钇掺杂量及电化学性能的研究,得到性能比较优良的LiY0.021Mn0.979O2化合物,其首次放电比容量为125.7 mA·h/g,100次循环以后,放电比容量达212.1 mA·h/g,远高于未掺杂材料的放电容量138 mA·h/g。交流阻抗测试结果表明, Y3+的掺入能降低材料的电化学反应阻抗和提高材料中Li+的扩散能力。     

混合锂盐及添加剂对镍锰酸锂电池性能的影响

采用不同的锂盐体系(LiBF_4、LiPF_6、LiODFB)及添加剂(T、FEC)对镍锰酸锂锂电池进行电性能测试。考察了镍锰酸锂作为正极材料在不同的锂盐电解液体系及添加剂下电池的循环性能、循环伏安曲线、阻抗的研究。结果表明:噻吩作为添加剂时,少量添加对电池的循环性能的改变越好;FEC的添加不影响电池容量,可以较好的保持电池的循环容量率;LiODFB的加入可以使电池的循环伏安曲线都具有单一的氧化还原峰,并使电池具有较好的循环性能。     

梯度包覆镍酸锂材料Li[Ni0.92Co0.04Mn0.04]O2的合成与研究

采用浓度梯度加料的方式,首先沉淀制备了核为Ni(OH)2、壳为镍钴锰氢氧化物浓度梯度包覆的复合前驱体,然后配锂高温焙烧,合成了梯度包覆的镍酸锂复合正极材料Li[Ni0.92Co0.04Mn0.04]O2。采用X射线衍射(XRD)、扫描电镜(SEM)、恒电流充放电测试等方法对材料的结构、表观形貌及电化学性能进行了表征。结果表明,该材料具有良好的六方单相层状α-NaFeO2结构,呈类球型状。切面元素线扫描显示该材料的包覆壳层中主要金属元素呈梯度变化。同时该新型梯度包覆的镍酸锂复合正极材料表现出了优越的电化学性能:在25℃下,2.8~4.3 V充放电范围,0.1C首次放电比容量可达198.3 mAh.g-1,循环40次容量保持96.8%;1C和2C倍率下放电比容量可达175 mAh.g-1和165.1 mAh.g-1。55℃下,该材料首次放电比容量可达236.1 mAh.g-1,循环40次容量仍能保持77.5%。     

铝锂混合掺杂尖晶石相Li_(1+x)Al_yMn_(2-y)O_4材料结构性能的研究

采用一种简单的合成工艺 ,将铝和锂混合掺入到主尖晶石相锰酸锂中 ,研究不同掺杂铝量对材料的初始容量及循环稳定性能的影响 .结果表明同时掺杂铝锂的材料要比单独掺杂铝或锂的循环稳定性好 .利用扫描电镜、粉末X_射线衍射仪、红外光谱仪对材料形貌及结构进行研究 ,结果表明所合成的掺杂铝锂材料颗粒细小、分布均匀 ,具有较好的结晶性能 ,较高的初始容量和良好的循环稳定性 ,其初始容量达 119mAh/g ,循环 2 0 0次后容量仍然保持在 10 6mAh/g     

层状LiMnO2的溶胶凝胶法合成及其改性

采用溶胶凝胶法合成了锂离子电池正极材料层状锰酸锂(o-L iMnO2),并对其进行了N i2+掺杂改性研究,优化了层状L iMnO2的合成路径及制备条件.采用XRD、充放电实验和交流阻抗测试方法研究了N i2+的掺入对o-L iMnO2充放电容量的影响.结果表明N i2+的掺入明显提高了锰酸锂的放电比容量和循环性能,抑制了循环过程中电池阻抗的增加.     

正极材料LiNi0.5Mn0.5-xCrxO2的低温燃烧合成

以LiNO3、Ni(NO3)2.6H2O、50%Mn(NO3)2溶液、Cr(NO3)3.9H2O和尿素为原料,采用低温燃烧法合成了LiNi0.5Mn0.5-xCrxO2,研究了回火温度、回火时间、锂过量和掺铬量对正极材料电化学性能的影响。结果表明,采用低温燃烧法合成LiNi0.5Mn0.5-xCrxO2的优化条件为:回火温度850℃、回火时间16h、锂过量15%,适宜掺铬量x=0.02。在优化条件下合成的正极材料具有α-NaFeO2型层状结构、球状形貌和良好的电化学性能,以0.1C速率在2.5～4.6V之间充放电,首次放电容量为179.9mAh/g,第50次循环放电容量仍保有171.0mAh/g,容量保持率达到95.1%。     

单斜层状结构锂离子电池正极材料LiY_xMn_(1-x)O_2的合成及其电化学性能

以Na2CO3、(CH3CO2)2Mn.4H2O、Y2O3和CH3COOLi.2H2O为原料,采用高温固相法经过2次灼烧和水热离子交换法得到一系列钇掺杂的LiMn1-xYxO2(x:0.01,0.02,0.03,0.05)化合物。通过XRD、XPS、循环伏安及恒电流充放电测试技术,研究了钇掺杂离子对合成正极材料结构及电化学性能的影响。结果表明,所得产物均具有单斜层状结构。合适的钇掺杂可以起到扩展锂离子脱嵌通道和稳定骨架结构的作用,钇离子的引入部分取代原有的三价锰离子,由于钇离子的离子半径较三价锰离子大,因此稀土掺杂锰酸锂材料的晶胞参数比未掺杂材料大,在一定程度上扩充了锂离子迁移的三维通道,更有利于锂离子的嵌入与脱嵌,提高单斜层状LiMnO2材料的电化学循环可逆性及循环稳定性。通过对所得化合物进行了钇掺杂量及电化学性能的研究,得到性能比较优良的LiY0.021Mn0.979O2化合物,其首次放电比容量为125.7mA.h/g,100次循环以后,放电比容量达212.1mA.h/g,远高于未掺杂材料的放电容量138mA.h/g。交流阻抗测试结果表明,Y3+的掺入能降低材料的电化学反应阻抗和提高材料中Li+的扩散能力。     

Sol-gel synthesis of K3InF6 and structural characterization of K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18

K₃InF₆ is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K₂InC₁₀O₁₀H₆F₉, K₃InC₁₂O₁₄H₄F₁₈ and K₃InC₁₂O₁₂F₁₈. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K₃InF₆ by decomposition at high temperature. The crystal structure of K₃InC₁₂O₁₄H₄F₁₈ is characterized by complex anions [In(CF₃COO)₄(OH_x)₂]^(5−2x)− and isolated [CF₃COOH_2−x]^(x−1)− molecules with x=2 or 1, surrounded by K⁺ cations. The crystal structure of K₃InC₁₂O₁₂F₁₈ is only constituted by complex anions [In(CF₃COO)₆]³⁻ and K⁺ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K₂InC₁₀O₁₀H₆F₉ and K₃InC₁₂O₁₂F₁₈ were also performed at room temperature on pulverized crystals.     

Li2O-TiO2-SiO2-P2O5和Li2O-TiO2-Al2O3-P2O5体系锂离子固体电解质的制备及性能研究

一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.     

A new 2212-type stair like structure: Bi14Sr21Fe12O61, m=5 member of the generic [Bi2Sr3Fe2O9]m[Bi4Sr6Fe2O16] family

A new oxide, Bi₁₄Sr₂₁Fe₁₂O_61, with a layered structure derived from the 2212 modulated type structure Bi₂Sr₃Fe₂O₉, was isolated. It crystallizes in the I2 space group, with the following parameters: a=16.58(3) Å, b=5.496(1) Å, c=35.27(2) Å and β=90.62°. The single crystal X-ray structure determination, coupled with electron microscopy, shows that this ferrite is the m=5 member of the [Bi₂Sr₃Fe₂O₉]_m[Bi₄Sr₆Fe₂O₁₆] collapsed family. This new collapsed structure can be described as slices of 2212 structure of five bismuth polyhedra thick along , shifted with respect to each other and interconnected by means of [Bi₄Sr₆Fe₂O₁₆] slices. The latter are the place of numerous defects like iron or strontium for bismuth substitution; they can be correlated to intergrowth defects with other members of the family.     

Synthesis, crystal structure, infrared and Raman spectra of Sr4Cu3(AsO4)2(AsO3OH)4·3H2O and Ba2Cu4(AsO4)2(AsO3OH)3

The two new compounds, Sr₄Cu₃(AsO₄)₂(AsO₃OH)₄·3H₂O (1) and Ba₂Cu₄(AsO₄)₂(AsO₃OH)₃(2), were synthesized under hydrothermal conditions. They represent previously unknown structure types and are the first compounds synthesized in the systems SrO/BaO-CuO-As₂O₅-H₂O. Their crystal structures were determined by single-crystal X-ray diffraction [space group C2/c, a=18.536(4) Å, b=5.179(1) Å, c=24.898(5) Å, β=93.67(3)°, V=2344.0(8) Å³, Z=4 for 1; space group P4₂/n, a=7.775(1) Å, c=13.698(3) Å, V=828.1(2) Å³, Z=2 for 2]. The crystal structure of 1 is related to a group of compounds formed by Cu²⁺-(XO₄)³⁻ layers (X=P⁵⁺, As⁵⁺) linked by M cations (M=alkali, alkaline earth, Pb²⁺, or Ag⁺) and partly by hydrogen bonds. In 1, worth mentioning is the very short hydrogen bond length, D···A=2.477(3) Å. It is one of the examples of extremely short hydrogen bonds, where the donor and acceptor are crystallographically different. Compound 2 represents a layered structure consisting of Cu₂O₈ centrosymmetric dimers crosslinked by As1φ₄ tetrahedra, where φ is O or OH, which are interconnected by Ba, As2 and hydrogen bonds to form a three-dimensional network. The layers are formed by Cu₂O₈ centrosymmetric dimers of CuO₅ edge-sharing polyhedra, crosslinked by As1O₄ tetrahedra. Vibrational spectra (FTIR and Raman) of both compounds are described. The spectroscopic manifestation of the very short hydrogen bond in 1, and ABC-like spectra in 2 were discussed.     

Raman scattering investigations on lanthanum-doped Bi4Ti3O12-SrBi4Ti4O15 intergrowth ferroelectrics

The ferroelectric ceramics of Bi₄Ti₃O₁₂, SrBi₄Ti₄O₁₅, and lanthanum-doped Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅ were synthesized, and their Raman spectra were investigated. La-doping resulted in the enlargement of remnant polarization of Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅. The structure of the Bi₂O₂ layers and TiO₆ octahedra of the intergrowth was found to be different from those of Bi₄Ti₃O₁₂ and SrBi₄Ti₄O₁₅. La³⁺ ions exhibit pronounced selectivity for the occupation of A site as La content is lower than 0.50, and tend to be incorporated into Bi₂O₂ layers when the La content is higher than 0.50. Lanthanum substitution brings about the structural phase transition in Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅. The variation of ferroelectric property may be attributed to combined contribution from the decreasing of the oxygen vacancies, the relaxation of the lattice distortion, the destroying of the insulation and the space charge compensation effects of the Bi₂O₂ slabs.     

Ion-beam irradiation of lanthanum compounds in the systems La2O3-Al2O3 and La2O3-TiO2

Thin crystals of La₂O₃, LaAlO₃, La_2/3TiO₃, La₂TiO₅, and La₂Ti₂O₇ have been irradiated in situ using 1 MeV Kr²⁺ ions at the Intermediate Voltage Electron Microscope-Tandem User Facility (IVEM-Tandem), Argonne National Laboratory (ANL). We observed that La₂O₃ remained crystalline to a fluence greater than 3.1×10¹⁶ ions cm⁻² at a temperature of 50 K. The four binary oxide compounds in the two systems were observed through the crystalline-amorphous transition as a function of ion fluence and temperature. Results from the ion irradiations give critical temperatures for amorphisation (T_c) of 647 K for LaAlO₃, 840 K for La₂Ti₂O₇, 865 K for La_2/3TiO₃, and 1027 K for La₂TiO₅. The T_c values observed in this study, together with previous data for Al₂O₃ and TiO₂, are discussed with reference to the melting points for the La₂O₃-Al₂O₃ and La₂O₃-TiO₂ systems and the different local environments within the four crystal structures. Results suggest that there is an observable inverse correlation between T_c and melting temperature (T_m) in the two systems. More complex relationships exist between T_c and crystal structure, with the stoichiometric perovskite LaAlO₃ being the most resistant to amorphisation.     

g-C_3N_4/CaTi_2O_5复合材料制备及其光催化性能

利用类石墨氮化碳(g-C_3N_4)和亚稳相钙钛氧化物(CaTi_2O_5)固相法制备C_3N_4/CaTi_2O_5复合材料。利用X射线衍射(XRD)、金相显微镜、扫描电子显微镜(SEM)及附带能谱分析仪(EDS)和N2吸附-脱附对样品的显微结构和比表面积进行检测分析,并用紫外-可见吸收光度计(UV-Vis)测试了样品的光吸收性能,研究C_3N_4与CaTi_2O_5物质的量之比(nC_3N_4/nCaTi_2O_5)对C_3N_4/CaTi_2O_5复合样品的物相结构和微观形貌的影响,同时考察C_3N_4/CaTi_2O_5复合样品在可见光照射下光催化降解罗丹明染料效果。实验结果表明:相比纯C_3N_4和CaTi_2O_5样品,C_3N_4/CaTi_2O_5复合样品在可见光下具有较高的光催化性能,随着nC_3N_4/nCaTi_2O_5增加,样品的光催化降解率随之增加而后降低,当nC_3N_4/nCaTi_2O_5=1∶1时,样品的光催化降解率达到最大值99.5%,并且循环重复利用5次后,样品的光催化剂降解率仍几乎保持不变。复合样品光催化性能提高主要归因于复合能级结构有效地抑制了电子和空穴复合所致。     

g-C3N4/CaTi2O5复合材料制备及其光催化性能

利用类石墨氮化碳（g-C₃N₄）和亚稳相钙钛氧化物（CaTi₂O₅）固相法制备C₃N₄/CaTi₂O₅复合材料。利用X射线衍射（XRD）、金相显微镜、扫描电子显微镜（SEM）及附带能谱分析仪（EDS）和N₂吸附-脱附对样品的显微结构和比表面积进行检测分析,并用紫外-可见吸收光度计（UV-Vis）测试了样品的光吸收性能,研究C₃N₄与CaTi₂O₅物质的量之比（n_C3N4/nCaTi₂O₅）对C₃N₄/CaTi₂O₅复合样品的物相结构和微观形貌的影响,同时考察C₃N₄/CaTi₂O₅复合样品在可见光照射下光催化降解罗丹明染料效果。实验结果表明：相比纯C₃N₄和CaTi₂O₅样品,C₃N₄/CaTi₂O₅复合样品在可见光下具有较高的光催化性能,随着n_C3N4/nCaTi₂O₅增加,样品的光催化降解率随之增加而后降低,当n_C3N4/nCaTi₂O₅=1：1时,样品的光催化降解率达到最大值99.5%,并且循环重复利用5次后,样品的光催化剂降解率仍几乎保持不变。复合样品光催化性能提高主要归因于复合能级结构有效地抑制了电子和空穴复合所致。     

Magnetic diphase nanostructure of ZnFe2O4/γ-Fe2O3

Magnetic diphase nanostructures of ZnFe₂O₄/γ-Fe₂O₃ were synthesized by a solvothermal method. The formation reactions were optimized by tuning the initial molar ratios of Fe/Zn. All samples were characterized by X-ray diffraction, thermogravimetric analysis, infrared spectroscopy, and Raman spectra. It is found that when the initial molar ratio of Fe/Zn is larger than 2, a diphase magnetic nanostructure of ZnFe₂O₄/γ-Fe₂O₃ was formed, in which the presence of ZnFe₂O₄ enhanced the thermal stability of γ-Fe₂O₃. Further increasing the initial molar ratio of Fe/Zn larger than 6 destabilized the diphase nanostructure and yielded traces of secondary phase α-Fe₂O₃. The grain surfaces of diphase nanostructure exhibited a spin-glass-like structure. At room temperature, all diphase nanostructures are superparamagnetic with saturation magnetization being increased with γ-Fe₂O₃ content.