新型复合正极材料5LiMn0.9Fe0.1PO4·Li3V2(PO4)3/C的制备及电化学性能研究

用固相法制备了5LiMn0.9Fe0.1PO4·Li3V2(PO4)3/C复合正极材料.采用XRD、SEM、TEM和电化学测试等对材料进行了表征.结果表明,复合材料由LiMn0.9Fe0.1PO4和Li3V2(PO4)3两相组成,不含其它杂质.Li3V2(PO4)3的加入使得LiMn0.9Fe0.1PO4的电化学性能得到极大地提高.该复合材料在0.05 C和1C倍率下的放电比容量分别为162.8 mAh·g-1和129.6mAh·g-1,在1C倍率下循环50次后的容量保持率为90.1;.     

Ti4+掺杂对磷酸钒锂材料结构和电化学性能的影响

分别采用溶胶-凝胶法和高温固相法制备锂离子电池正极材料Li3V1.93 Ti0 05(PO4) 3/C,研究Ti4+掺杂对Li3 V2(PO4)3材料结构、形貌和电化学性能的影响.结果表明:利用溶胶-凝胶法和高温固相法均得到单斜晶系结构,且无杂相存在,少量Ti4掺杂并未影响材料的结构形貌,但显著改善了电化学性能.溶胶-凝胶法掺杂Ti4+试样在0.2C和12 C放电比容量分别为129 mAh·g-1和102 mAh·g-1,明显高于高温固相法掺杂Ti4+试样,且循环性能良好.研究表明利用溶胶-凝胶法掺杂是一种改善离子掺杂效果的有效路径.     

溶胶-凝胶法合成3LiMnPO4·Li3V2(PO4)3及其电化学性能研究

以柠檬酸为络合剂,聚乙二醇(PEG)为表面活性剂,偏钒酸铵、乙酸锰、磷酸二氢铵、氢氧化锂为原料,采用溶胶-凝胶法合成了xLiMnPO4·yLi3V2(PO4)3锂离子电池复合正极材料.采用X射线衍射(XRD)、扫描电镜(SEM)对其晶体结构和微观形貌进行表征,结果表明在700℃下烧结15 h合成的3LiMnPO4·Li3V2(PO4)3为结晶良好的两相结构,颗粒粒径相对较小且分布均匀.电化学性能研究表明,3LiMnPO4·Li3V2(PO4)3在室温0.2C倍率下首次充放电容量分别为148.2 mAh/g和141.5 mAh/g,循环50次后放电容量为136.7 mAh/g.     

以酚醛树脂为碳源合成锂离子电池正极材料Li3V2 (PO4)3/C

以酚醛树脂为碳源,分别采用了固相法和溶胶凝胶法合成了锂离子电池正极材料Li3V2(PO4)3/C.结果表明,高分子材料酚醛树脂是一种优良的碳源材料,其热解后得到的导电网络能够有效的提高Li3V2(PO4)3的电化学性能;两种试样的充放电曲线和交流阻抗图谱体现出了试样良好的可逆性,其极化程度很低,电荷转移电阻小;而相对于固相法来讲,溶胶凝胶法和表面活性剂CTAB(十六烷基三甲基溴化铵)的共同作用能够有效的将颗粒粒径控制在纳米级别.用这种方法合成的试样在15 C下充放电比容量也能高于90 mAh/g,5C倍率下循环50次比容量无衰减,证明了以酚醛树脂为碳源并采用溶胶凝胶法合成的试样具有很好的倍率性能与循环性能.     

一步水热法制备钠离子电池正极材料Na3V2(PO4)2F3及其性能研究

采用一步水热法制备了钠离子电池正极材料Na3V2(PO4)2F3,用XRD、SEM、恒流充放电等对样品进行了表征.研究表明,络合剂种类对Na3V2(PO4)2F3的结构、形貌及电化学性能有重大影响,以抗坏血酸、柠檬酸、草酸和酒石酸为络合剂制备的样品分别为小立方体、球形、大立方体和不规则球状,除以酒石酸为络合剂制备的样品为无定形结构外,其余样品均结晶良好.其中以抗坏血酸为络合剂制备的样品结晶度最高且电化学性能最优,该样品在0.05 C和0.5C倍率下的首次放电比容量为112.0 mAh/g和92.5 mAh/g,且具有良好的倍率性能和循环性能.     

3LiMnPO4·Li3V2（PO4）3正极材料的制备及其电化学性能研究

以五氧化二钒干凝胶、碳酸锰、磷酸二氢铵、碳酸锂、乙炔黑为原料,采用固相法在相对较低的温度条件下合成了x Li Mn PO4·y Li3V2(PO4)3锂离子电池复合正极材料。采用X射线衍射(XRD)、扫描电镜(SEM)对其晶体结构和表面形貌进行表征。结果表明,750℃下烧结15 h合成的3Li Mn PO4·Li3V2(PO4)3为结晶良好的两相结构,颗粒粒径较小且分布比较均匀,其在室温、0.2 C倍率下首次充放电容量分别为144.8 m Ah/g和139.8 m Ah/g,循环50次后容量为130.5 m Ah/g。     

负极材料Li4Ti5O12的制备与性能研究

利用纳米二氧化钛(P25)粉为钛源,Li2CO3为锂源,采用固相法及高能球磨法制备亚微米级尖晶石Li4Ti5O12.将Li4Ti5O12与碳纳米管(CNTs)制备成复合电极作为工作电极与锂片组成电池进行电化学性能测试.通过SEM,XRD等表征材料形貌、结构及粒径分布,通过充放电测试表征其电化学性能.结果表明,在800℃合成温度及8h合成时间制备条件下可以得到小尺寸且颗粒均匀的亚微米晶体Li4Ti5O12,且合成的产物电化学性能最佳.在800℃及8h合成条件下,产物首次充放电容量分别为188.0 mAh/g和189.1 mAh/g,首次充放效率为99.4％,且具有良好的可逆性.     

新型锂离子电池复合负极材料3Li4Ti5O12·NiO的制备及性能研究

采用喷雾干燥法合成了3Li4Ti5O12·NiO复合负极材料.XRD结果表明,复合NiO没有改变Li4Ti5On的晶体结构.SEM结果表明,样品为直径0.5～3 μm的球形颗粒.电化学测试结果表明,3Li4Ti5O12·NiO较Li4Ti5O12倍率性能和循环性能得到极大地提高.该复合材料在0.1C、1C和20 C倍率下的放电比容量分别为372.8 mAh·g-1、252.6 mAh·g-1和204.8 mAh·g-1,在20C倍率下循环300次后的容量保持率为98.7;.     

焙烧温度对Li[Mn1/3Ni1/3CO1/3]O2结构及电化学性能影响

采用碳酸盐共沉淀法制备了Li[Mn1/3Ni1/3Co1/3]O2,研究了前驱体的焙烧温度对材料结构和电化学性能的影响.XRD测试结果表明,800℃下焙烧得到的样品具有较好的层状结构和较低的阳离子混排程度.SEM测试表明合成材料具有球状形貌,平均粒径可达5μm,组成它的一次颗粒粒径平均为200nm.在2.8～4.3V(vs.Li/Li+)0.2C条件下进行充放电测试,800℃下合成的样品的首次放电比容量最高(159.06mAh·g-1),容量损失最小,循环50次后能保持初始放电比容量的95.7;.EIS分析结果表明,800℃焙烧的样品的电化学活性最好.     

Co掺杂对富锂锰基正极材料Li1.2Ni0.2Mn0.6O2电化学性能的影响

本文以醋酸盐为原料,采用溶胶凝胶法制备富锂锰基固溶体正极材料Li1.2Ni0.2Mn0.6O2.研究Co掺杂后对Li1.2 Ni0.2-x/2Mn0.6-x/2 CoxO2(x=0,0.01,0.02,0.05)材料结构以及电化学性能的影响.XRD和SEM测试表明:Co掺杂后样品结构未发生改变,均属于富锂锰基正极材料.电化学测试表明:Co掺杂能改善材料的倍率性能,提高材料的放电比容量.其中,x=0.02的材料Li1.2Ni0.19Mn0.59Co0.02O2具有最优异的电化学性能,0.05 C下的首次放电比容量由未掺杂的的217 mAh·g-1提升至332.6 mAh·g-1;0.1 C下经40次循环后放电比容量为171.6 mAh·g-1,保持率为85.5;.     

The structures of three trimethylarsine-boron trihalide adducts: (CH3)3AsBCl3, (CH3)3AsBBr3, and (CH3)3AsBI3

An X-ray structure analysis of three trimethylarsine-boron trihalide adducts has been undertaken. Crystals of (CH₃)₃AsBCl₃ and (CH₃)₃AsBBr₃ are monoclinic with space groupP2₁/m (No. 11) withZ=2 while those of (CH₃)₃AsBI₃ are orthorhombic with space groupPnma (No. 62) withZ=4. For (CH₃)₃AsBCl₃,a=6.497(3) Å,b=10.735(3) Å,c=7.070(2) Å,=111.8(3)°,V=458.4(3) ų,R=0.0343. For (CH₃)₃AsBBr₃,a=6.672(4) Å,b=11.135(7) Å,c=7.199(4) Å,=111.5(1)°,V=497.7(5) ų,R=0.0434. For (CH₃)₃ÅsBI₃,a=13.113(7) Å,b=11.733(5) Å,c=7.387(3) Å,V=1136.5(5) ų,R=0.0329. The As-B bond lengths are 2.065(6), 2.04(1), and 2.03(1) Å, respectively, for the chloride, bromide, and iodide. These and other structural parameters are discussed with reference to previous predictions based on vibrational spectra and previous structural studies on the trimethyl-phosphine and trimethylamine adducts.     

Crystal and molecular structures of three trimethylamine-boron halide adducts: (CH3)3NBCl3, (CH3)3NBBr3, and (CH3)3NBI3

X-ray diffraction data from single crystals of the trimethylamine complexes of the three boron halides, BCl₃, BBr₃, and BI₃, lead to aP2₁/m monoclinic cell containing two molecules for each complex. The unit cell dimensions area = 6·68(1),b = 10·247(3),c = 6·502(6) Å, =116·2(1)° (chloro);a = 6·86(1),b = 10·612(4),c = 6·737(6) Å, = 115·8(1)° (bromo);a = 6·92(2),b = 10·86(1),c = 7·147(6) Å, = 93·9(1)° (iodo). The structures were solved by three-dimensional sharpened Patterson functions and show only the chloro and bromo compounds to be isomorphous. Refinement of 662,718 and 954 observed reflexions for the chloro, bromo and iodo complexes, respectively, using anisotropic thermal parameters yielded conventionalR factors of 0·045, 0·087 and 0·054.The molecules are shown to possess a B—N dative bond, a staggered conformation, and effective 3m (C _3v) symmetry. Average C—N bond lengths are 1·52(1) Å for all three complexes. Boronhalogen bond lengths average 1·864(4), 2·04(2) and 2·28(2) Å, while B—N bond distances are 1·609(6), 1·60(2) and 1·58(3) Å, respectively, for the chloro through iodo compounds. Bond angles are approximately tetrahedral with the C—N—C angle decreasing by several degrees in the Cl Br I series.Based in part on a dissertation submitted by Patty H. Clippard to the Rackham School of Graduate Studies of the University of Michigan, January 1969 in partial fulfillment of the requirements of the Ph.D. Degree.     

Second harmonic generation properties of Ca3(O3C3N3)2 ‐Sr3(O3C3N3)2 solid solutions

Solid solutions of the second harmonic generation (SHG) materials Ca₃(O₃C₃N₃)₂ (CCY) and Sr₃(O₃C₃N₃)₂ (SCY) were prepared via exothermic solid state metathesis reactions from appropriate amounts of the corresponding metal chlorides and potassium cyanate at 525 °C. The change in SHG intensity caused by the successive cation substitution is reported. Differential thermal analyses are used to explore the SCY–K(OCN) phase diagram as a medium for the growth of SCY crystals.     

Crystal Growth and Spectroscopic Characterisation of BiB3O6:RE3+ (RE3+ = Pr3+, Nd3+, Gd3+, Er3+, Tm3+)

Large single crystals of optical quality of BiB₃O₆:RE³⁺ (RE³⁺ = Pr³⁺, Nd³⁺, Gd³⁺, Er³⁺, Tm³⁺) were grown from nearly stoichiometric melts using the top‐seeding growth technique to dimensions up to 12 x 12 x 18 mm³. Absorption spectra were measured in the wavelength range from 10000 cm^‐1 to 30000 cm^‐1 with an absorption spectrometer to estimate the doping concentration of RE³⁺. For the determination of the phonon energies and the quenching behaviour of the host lattice IR and Raman spectra were recorded.     

Infrared vibrational Modes in Tl3SbS3, Tl3AsS3, and Tl3AsSe3 crystals

Reflectivity spectra of Tl₃SbS₃, Tl₃AsS₃, and Tl₃AsSe₃ crystals have been investigated in the wave number range 50–600 cm⁻¹ for the polarizations E∥c and E⟂c. The fundamental phonon parameters, the limiting dielectric constants ϵ_∞ and ϵ_S and the reflectivity spectra contours have been calculated by using classical dispersion relations for both E∥c and E⟂c configurations. The Szigeti effective charges and the relative ion charges of As, Tl, Sb, Se, S anions and cations have been calculated in dependence on the incident light polarization.     

Growth and characteristic of Sr3Tb(BO3)3 crystal

A new borate single crystal of Sr₃Tb(BO₃)₃ with dimension Ф20×25 mm² has been grown by the Czochralski method. The grown crystal was characterized by DTA–TGA, FTIR and X-ray powder diffraction analysis. The results showed the crystal with [BO₃]^3? is congruently melting at 1351.35 °C which belongs to hexagonal structure. The hardness of Sr₃Tb(BO₃)₃ crystal is 422.5 VDH, and is equal to 5.0 moh. The thermal expansion coefficients were determined to be 2.08×10^?5/°C along (1 0 0) direction and 7.43×10^?6/°C along (0 0 1) direction and the transmission spectrum was measured in 320–1800 nm at room temperature. The magnetic properties of the single crystal were studied which showed its paramagnetism and magnetic anisotropy. The specific Faraday rotation of single crystal was measured at room temperature in 532, 633, and 1064 nm wavelength. The Verdet constants and magneto-optical figures of merit were investigated. The primary emphasis is laid to explore a new magneto-optical material, all the magneto-optical properties of Sr₃Tb(BO₃)₃ are comparing to the ones of TGG.     

Photoacoustic Spectra of Pr3+, Nd3+, Gd3+ Acetate Complexes

The crystals of the complexes Pr(Ac)₃ · 4 H₂O, Nd(Ac)₃ · 4 H₂O, Gd(Ac)₃ · 4 H₂O were synthesized and their Pa spectra determined firstly. Their PA spectra and absorption are interpreted. The fluorescence properties of Pr³⁺, Nd³⁺, Gd³⁺ and the relaxation process models were studied by their PA spectra.     

Tb3+,Yb3+共掺杂LuBO3荧光粉的下转换发光

利用水热法成功合成了近红外量子剪裁荧光粉LuBO3∶15;Tb3+,x; Yb3+(x=0,1,2,4,8,12).通过X射线衍射(XRD)、光致发光谱(PL)、激发谱(PLE)和荧光寿命测试了合成物质的物相结构与发光性质.在286 nm(Tb3+∶7 F6→5D)紫外光激发下,观察到了Tb3∶5D4→7Fj(J=6,5,4,3)可见波段特征发射光和Yb3+:2F5/2→2F7/2的近红外光.研究了Yb3+浓度与激发发射光谱和荧光寿命之间的关系,表明Tb3+和Yb3+之间存在能量传递.当Tb3和Yb3+掺杂摩尔浓度分别为15;和2;时,近红外发射最强.计算得知,其最大下转换量子效率为160.74;.     

Melting temperatures of NaClO3-NaBrO3 mixed crystals

The melting points of mixed crystals of sodium chlorate and sodium bromate have been determined. The variation of melting point with composition is non-linear with negative deviations from linearity. This negative deviation from linearity is attributed to a possible increase in the vacancy concentration in mixed crystals as compared to the pure end crystals.