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1.
High-pressure synthesis in an oxygen-rich atmosphere yields solid solutions between LiNiO2 and Li2NiO3 over the whole concentration range. Structural characterization of the high-pressure oxides was performed using powder XRD, SEM analysis, IR spectroscopy, EPR spectroscopy at 9.23 and 115 GHz and magnetic susceptibility measurements. The crystal structure of Li[LixNi1−x]O2 ,, changes from trigonal R-3m to monoclinic C2/m at Li-to-Ni ratio of 2 (or ). The incorporation of Li into NiO2-layers causes a decrease in the mean Li-O and Ni1-xLix-O bond distance. Li and Ni ions in the mixed Ni1-xLixO2-layers display a tendency to order at a short length scale in such a way that mimics the Li1/3Ni2/3-arrangment of the end Li[Li1/3Ni2/3]O2 composition. The charge distribution in these oxides proceeds via Ni3+ and Ni4+ ions.  相似文献   

2.
X-ray diffraction patterns of Li[Li(1−2x)/3NixMn2/3−x/3]O2 show reflections between 20° and 35°, 2θ (CuKα) due to Li2MnO3-like ordering of the transition metal (Ni, Mn and Li) layers. The ordering is rarely perfect, resulting in characteristic broadening and changes in the intensities of these reflections. 6Li MAS NMR studies of Li2MnO3 show that the [Li1/3Mn2/3] layers are well ordered, the disorder arising from the stacking of the layers in the c-direction. DIFFaX was used to model the Li2MnO3 XRD data and extract the stacking fault frequency. The results show that even well-ordered cation layers may show only weak or no superstructure reflections, if there is no or little ordering in the c-direction.  相似文献   

3.
The transport properties and lithium insertion mechanism into the first mixed valence silver-copper oxide AgCuO2 and the B-site mixed magnetic delafossite AgCu0.5Mn0.5O2 were investigated by means of four probes DC measurements combined with thermopower measurements and in situ XRD investigations. AgCuO2 and AgCu0.5Mn0.5O2 display p-type conductivity with Seebeck coefficient of Q=+2.46 and +78.83 μV/K and conductivity values of σ=3.2×10−1 and 1.8×10−4 S/cm, respectively. The high conductivity together with the low Seebeck coefficient of AgCuO2 is explained as a result of the mixed valence state between Ag and Cu sites. The electrochemically assisted lithium insertion into AgCuO2 shows a solid solution domain between x=0 and 0.8Li+ followed by a plateau nearby 1.7 V (vs. Li+/Li) entailing the reduction of silver to silver metal accordingly to a displacement reaction. During the solid solution, a rapid structure amorphization was observed. The delafossite AgCu0.5Mn0.5O2 also exhibits Li+/Ag+ displacement reaction in a comparable potential range than AgCuO2; however, with a prior narrow solid solution domain and a less rapid amorphization process. AgCuO2 and AgCu0.5Mn0.5O2 provide a discharge gravimetric capacity of 265 and 230 mA h/g above 1.5 V (vs. Li+/Li), respectively, with no evidence of a new defined phases.  相似文献   

4.
Cathode materials Li[CoxMn1−x]O2 for lithium secondary batteries have been prepared by a new route—precursor method of layered double hydroxides (LDHs). In situ high-temperature X-ray diffraction (HT-XRD) and thermogravimetric analysis coupled with mass spectrometry (TG-MS) were used to monitor the structural transformation during the reaction of CoMn LDHs and LiOH·H2O: firstly the layered structure of LDHs transformed to an intermediate phase with spinel structure; then the distortion of the structure occurred with the intercalation of Li+ into the lattice, resulting in the formation of layered Li[CoxMn1−x]O2 with α-NaFeO2 structure. Extended X-ray absorption fine structure (EXAFS) data showed that the Co-O bonding length and the coordination number of Co were close to those of Mn in Li[CoxMn1−x]O2, which indicates that the local environments of the transitional metals are rather similar. X-ray photoelectron spectroscopy (XPS) was used to measure the oxidation state of Co and Mn. The influences of Co/Mn ratio on both the structure and electrochemical property of Li[CoxMn1−x]O2 have been investigated by XRD and electrochemical tests. It has been found that the products synthesized by the precursor method demonstrated a rather stable cycling behavior, with a reversible capacity of 122.5 mAh g−1 for the layered material Li[Co0.80Mn0.20]O2.  相似文献   

5.
Layered LiNi0.4Co0.2Mn0.4O2, Li[Li0.182Ni0.182Co0.091Mn0.545]O2, Li[Li1/3Mn2/3]O2 powder materials were prepared by rheological phase method. XRD characterization shows that these samples all have analogous structure to LiCoO2. Li[Li0.182Ni0.182Co0.091Mn0.545]O2 can be considered to be the solid solution of LiNi0.4Co0.2Mn0.4O2 and Li[Li1/3Mn2/3]O2. Detailed information from XRD, ex situ XPS measurement and electrochemical analysis of these three materials reveals the origin of the irreversible plateau (4.5 V) of Li[Li0.182Ni0.182Co0.091Mn0.545]O2 electrode. The irreversible oxidation reaction occurred in the first charging above 4.5 V is ascribed to the contribution of Li[Li1/3Mn2/3]O2 component, which maybe extract Li+ from the transition layer in Li[Li1/3Mn2/3]O2 or Li[Li0.182Ni0.182Co0.091Mn0.545]O2 through oxygen release. This step also activates Mn4+ of Li[Li1/3Mn2/3]O2 or Li[Li0.182Ni0.182Co0.091Mn0.545]O2, it can be reversibly reduced/oxidized between Mn4+ and Mn3+ in the subsequent cycles.  相似文献   

6.
运用共沉淀和元素化学沉积相结合的方法,制备出了具有Ag/C 包覆层的层状富锂固溶体材料Li[Li0.2Mn0.54Ni0.13Co0.13]O2. 通过X 射线衍射(XRD)、场发射扫描电子显微镜(SEM)、透射电子显微镜(TEM)、恒流充放电、循环伏安(CV),电化学阻抗谱(EIS)和X 射线能量散射谱(EDS)方法,研究了Ag/C 包覆层对Li[Li0.2Mn0.54Ni0.13Co0.13]O2电化学性能的影响. 结果表明,Ag/C 包覆层的厚度约为25 nm,Ag/C 包覆在保持了固溶体材料α-NaFeO2 六方层状晶体结构的前提下,显著地改善了Li[Li0.2Mn0.54Ni0.13Co0.13]O2 的电化学性能. 在2.0-4.8 V(vs Li/Li+)的电压范围内,首次放电(0.05C)容量由242.6 mAh·g-1提高到272.4 mAh·g-1,库仑效率由67.6%升高到77.4%;在0.2C倍率下,30 次循环后,Ag/C 包覆的电极材料容量为222.6 mAh·g-1,比未包覆电极材料的容量高出14.45%;包覆后的电极材料在1C下的容量仍为0.05C下的81.3%. 循环伏安及电化学交流阻抗谱研究表明,Ag/C包覆层抑制了材料在充放电过程中氧的损失,有效降低了Li[Li0.2Mn0.54Ni0.13Co0.13]O2颗粒的界面膜电阻与电化学反应电阻.  相似文献   

7.
Layered Li[Li0.16Ni0.21Mn0.63]O2 and Li[Li0.2Ni0.2Mn0.6]O2 compounds were successfully synthesized by radiated polymer gel (RPG) method. The effect of deficient Li on the structure and electrochemical performance was investigated by means of X-ray diffraction, X-ray absorption near-edge spectroscopy and electrochemical cell cycling. The reduced Ni valence in Li[Li0.16Ni0.21Mn0.63]O2 leads to a higher capacity owing to faster Li+ chemical diffusivity relative to the baseline composition Li[Li0.2Ni0.2Mn0.6]O2. Cyclic voltammograms (CV) and a simultaneous direct current (DC) resistance measurement were also performed on Li/Li[Li0.16Ni0.21Mn0.63]O2 and Li/Li[Li0.2Ni0.2Mn0.6]O2 cells. Li[Li0.16Ni0.21Mn0.63]O2 shows better electrochemical performance with a reversible capacity of 158 mA hg−1 at 1C rate at 20 °C.  相似文献   

8.
9.
A new vanado-molybdate LiMg3VMo2O12 has been synthesized, the crystal structure determined an ionic conductivity measured. The solid solution Li2−zMg2+zVzMo3−zO12 was investigated and the structures of the z=0.5 and 1.0 compositions were refined by Rietveld analysis of powder X-ray (XRD) and powder neutron diffraction (ND) data. The structures were refined in the orthorhombic space group Pnma with a∼5.10, b∼10.4 and c∼17.6 Å, and are isostructural with the previously reported double molybdates Li2M2(MoO4)3 (M=M2+, z=0). The structures comprise of two unique (Li/Mg)O6 octahedra, (Li/Mg)O6 trigonal prisms and two unique (Mo/V)O4 tetrahedra. A well-defined 1:3 ratio of Li+:Mg2+ is observed in octahedral chains for LiMg3VMo2O12. Li+ preferentially occupies trigonal prisms and Mg2+ favours octahedral sheets. Excess V5+ adjacent to the octahedral sheets may indicate short-range order. Ionic conductivity measured by impedance spectroscopy (IS) and differential scanning calorimetry (DSC) measurements show the presence of a phase transition, at 500-600 °C, depending on x. A decrease in activation energy for Li+ ion conductivity occurs at the phase transition and the high temperature structure is a good Li+ ion conductor, with σ=1×10−3-4×10−2 S cm−1 and Ea=0.6 to 0.8 eV.  相似文献   

10.
0IntroductionMany efforts have been made to develop newmaterials as an alternative to LiCoO2due to the rela-tively high cost and toxicity of Co.Much attention hasbeen paid to layered structure cathode materials suchas LiMnO2and LiNiO2due to their lower co…  相似文献   

11.
LiMnC2O4(Ac) precursor in which Li+ and Mn2+ were amalgamated in one molecule was prepared by solid-state reaction at room-temperature using manganese acetate, lithium hydroxide and oxalic acid as raw materials. By thermo-decomposition of LiMnC2O4(Ac) at various temperatures, a series of Li1+y[Mn2−xLix]16dO4 spinels were prepared with Li2MnO3 as impurities. The structure and phase transition of these spinels were investigated by XRD, TG/DTA, average oxidation state of Mn and cyclic voltammeric techniques. Results revealed that the Li-Mn-O spinels with high Li/Mn ratio were unstable at high temperature, and the phase transition was associated with the transfer of Li+ from octahedral 16c sites to 16d sites. With the sintering temperature increasing from 450 to 850 °C, the phase structure varied from lithiated-spinel Li2Mn2O4 to Li4Mn5O12-like to LiMn2O4-like and finally to rock-salt LiMnO2-like. A way of determining x with average oxidation state of Mn and the content of Li2MnO3 was also demonstrated.  相似文献   

12.
为提高锂离子电池正极材料Li[Li0.2Ni0.2Mn0.6]O2的首次充放电效率,对固相法合成的该材料进行了酸浸的改性研究。通过X射线衍射(XRD)、扫描电子显微镜(SEM)对所得样品的结构、形貌进行了表征。结果表明,Li[Li0.2Ni0.2Mn0.6]O2经过酸处理后,首次放电效率得到了较大的提高,但是放电中值电压明显下降。其中,0.5 mol.L-1的硝酸浸泡5 h的效果最佳,首次放电效率达到了86.7%,同时放电容量达到最大值的循环次数大大减少。酸浸改性的原因被归结于材料表面出现了富锂尖晶石结构Li4Mn5O12相。  相似文献   

13.
Lithium-nickel-manganese oxides (Li1+x(Ni1/2Mn1/2)1−xO2, x=0 and 0.2), having different cationic distributions and an oxidation state of Ni varying from 2+ to 3+, were formed under a high-pressure (3 GPa). The structure and cationic distribution in these oxides were examined by powder X-ray diffraction, infrared (IR) and electron paramagnetic resonance (EPR) in X-band (9.23 GHz) and at higher frequencies (95 and 285 GHz). Under a high pressure, a solid-state reaction between NiMnO3 and Li2O yields LiNi0.5Mn0.5O2 with a disordered rock-salt type structure. The paramagnetic ions stabilized in this oxide are mainly Ni2+ and Mn4+ together with Mn3+ (about 10%). The replacement of Li2O by Li2O2 permits increasing the oxidation state of Ni ions in lithium-nickel-manganese oxides. The higher oxidation state of Ni ions favours the stabilization of the layered modification, where the Ni-to-Mn ratio is preserved: Li(Li0.2Ni0.4Mn0.4)O2. The paramagnetic ions stabilized in the layered oxide are mainly Ni3+ and Mn4+ ions. The disordered and ordered phases display different intercalation properties in respect of lithium. The changes in local Ni,Mn-environment during the electrochemical reaction are discussed on the basis of EPR and IR spectroscopy.  相似文献   

14.
A series of lithium–manganese–nickel-oxide compositions that can be represented in three-component notation, xLi[Mn1.5Ni0.5]O4 · (1  x){Li2MnO3 · Li(Mn0.5Ni0.5)O2}, in which a spinel component, Li[Mn1.5Ni0.5]O4, and two layered components, Li2MnO3 and Li(Mn0.5Ni0.5)O2, are structurally integrated in a highly complex manner, have been evaluated as electrodes in lithium cells for x = 1, 0.75, 0.50, 0.25 and 0. In this series of compounds, which is defined by the Li[Mn1.5Ni0.5]O4–{Li2MnO3 · Li(Mn0.5Ni0.5)O2} tie-line in the Li[Mn1.5Ni0.5]O4–Li2MnO3–Li(Mn0.5Ni0.5)O2 phase diagram, the Mn:Ni ratio in the spinel and the combined layered Li2MnO3 · Li(Mn0.5Ni0.5)O2 components is always 3:1. Powder X-ray diffraction patterns of the end members and the electrochemical profiles of cells with these electrodes are consistent with those expected for the spinel Li[Mn1.5Ni0.5]O4 (x = 1) and for ‘composite’ Li2MnO3 · Li(Mn0.5Ni0.5)O2 layered electrode structures (x = 0). Electrodes with intermediate values of x exhibit both spinel and layered character and yield extremely high capacities, reaching more than 250 mA h/g with good cycling stability between 2.0 V and 4.95 V vs. Li° at a current rate of 0.1 mA/cm2.  相似文献   

15.
Mixed crystals of Li[Kx(NH4)1−x]SO4 have been obtained by evaporation from aqueous solution at 313 K using different molar ratios of mixtures of LiKSO4 and LiNH4SO4. The crystals were characterized by Raman scattering and single-crystal and powder X-ray diffraction. Two types of compound were obtained: Li[Kx(NH4)1−x]SO4 with x?0.94 and Li2KNH4(SO4)2. Different phases of Li[Kx(NH4)1−x]SO4 were yielded according to the molar ratio used in the preparation. The first phase is isostructural to the room-temperature phase of LiKSO4. The second phase is the enantiomorph of the first, which is not observed in pure LiKSO4, and the last is a disordered phase, which was also observed in LiKSO4, and can be assumed as a mixture of domains of two preceding phases. In the second type of compound with formula Li2KNH4(SO4)2, the room-temperature phase is hexagonal, symmetry space group P63 with cell-volume nine times that of LiKSO4. In this phase, some cavities are occupied by K+ ions only, and others are occupied by either K+ or NH4+ at random. Thermal analyses of both types of compounds were performed by DSC, ATD, TG and powder X-ray diffraction. The phase transition temperatures for Li[Kx(NH4)1−x]SO4x?0.94 were affected by the random presence of the ammonium ion in this disordered system. The high-temperature phase of Li2KNH4(SO4)2 is also hexagonal, space group P63/mmc with the cell a-parameter double that of LiKSO4. The phase transition is at 471.9 K.  相似文献   

16.
The chemical stability of the layered Li1−xCoO2 and Li1−xNi0.85CoO.15O2 cathodes is compared by monitoring the oxygen content with lithium content (1−x) in chemically delithiated samples. The Li1−xCoO2 system tends to lose oxygen from the lattice at deep lithium extraction while the Li1−xNi0.85Co0.15O2 system does not lose oxygen at least for (1−x)>0.3. This difference seems to result in a lower reversible (practical) capacity (140 mA h/g) for LiCoO2 compared to that for LiNi0.85Co0.15O2 (180 Ma h/g). The loss of significant amount of oxygen leads to a sliding of oxide layers and the formation of a major P3 and a minor O1 phase for the end member CoO2−δ with δ=0.33. In contrast, Ni0.85Co0.15O2−δ with a small amount of δ=0.1 maintains the initial O3 layer structure.  相似文献   

17.
顾大明  谢颖  史鹏飞  付宏刚 《化学学报》2006,64(12):1223-1227
>为获得综合性能更好的锂离子二次电池正极材料, 分析了Co掺杂对LixNiO2电化学性能的影响. 采用密度泛函DFT理论对LixNiO2和LixNi0.5Co0.5O2的平均放电电压和态密度进行了计算. 同时, 用共沉淀法制备了LixNiO2和LixNi0.5Co0.5O2锂离子二次电池正极材料, 并对其进行了XRD结构分析和恒流充放电测试. 实验和计算结果表明: 随锂离子嵌入正极(电池放电), 电池的电压逐渐降低, 材料的态密度峰向低能量方向移动; 与LixNiO2相比, LixNi0.5Co0.5O2的电压平台相对较高(当0.25≤x≤0.5), 而且在Li嵌/脱时, LixNi0.5Co0.5O2的结构变化相对较小; Co离子的掺入, 减小了NiO6八面体的畸变度, 使材料的电化学稳定性得以提高. 在钴掺杂镍酸锂体系中, NiO6和CoO6具有相互的稳定作用.  相似文献   

18.
A comparative study on the oxidation and charge compensation in the AxCoO2−δ systems, A=Na (x=0.75, 0.47, 0.36, 0.12) and Li (x=1, 0.49, 0.05), using X-ray absorption spectroscopy at O 1s and Co 2p edges is reported. Both the O 1s and Co 2p XANES results show that upon removal of alkali metal from AxCoO2−δ the valence of cobalt increases more in LixCoO2−δ than in NaxCoO2−δ. In addition, the data of O 1s XANES indicate that charge compensation by oxygen is more pronounced in NaxCoO2−δ than in LixCoO2−δ.  相似文献   

19.
LiMg0.5Mn1.5O4的合成及对Li+的离子交换选择性   总被引:8,自引:0,他引:8  
锂及其化合物在航空航天、化工、医药、空调、高能电池和热核反应等方面都有广泛应用,对锂及其化合物的需求与日俱增。我国液体锂资源非常丰富,开发利用其中的锂资源具有重要意义。从盐湖水、地下卤水、盐田母液、油气田水等咸水资源中提取锂的方法有碳酸盐沉淀法、离子交换法、萃取法等。离子  相似文献   

20.
采用高温固相合成法制备了Li[Ni(1-x)/3Mn(1-x)/3Co(1-x)/3Mox]O2 (x=0, 0.005, 0.01, 0.02). 对它们进行了XRD, SEM, 循环伏安及充放电容量测试, 结果发现, 掺杂x=0.01 Mo的样品具有较高的嵌锂容量和良好的循环稳定性, 在20 mA/g放电电流密度和2.3~4.6 V的电压范围内具有211.6 mAh/g的首次放电比容量, 循环50周后放电比容量仍能达到185.9 mAh/g, 容量损失为12.1%.  相似文献   

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