Comparative study of LiNi0.05Mn1.95O4 powders prepared by different materials for Li-ion battery

LiNi_0.05Mn_1.95O₄ powders were prepared by manganese tetraoxide (MTO) and electrolytic manganese dioxide (EMD). The phase identification, surface morphology, and electrochemical properties of the prepared powders were studied by X-ray diffraction, scanning electron microscopy, cyclic voltammetry, and galvanostatic charge?Cdischarge experiments. Compared to LiNi_0.05Mn_1.95O₄ powders prepared by EMD, LiNi_0.05Mn_1.95O₄ powders prepared by MTO show better crystallinity. Both powders possess a typical cubic structure with uniform particle size. The specific capacity and coulombic efficiency of LiNi_0.05Mn_1.95O₄ powders prepared by MTO are higher than the one prepared by EMD. The capacity retention of LiNi_0.05Mn_1.95O₄ powders prepared by MTO cycled 30 times at room temperature and 55?°C are 98.3% and 90.6%, respectively, which are much higher than those of 86.63% and 77.7% for the one prepared by EMD. LiNi_0.05Mn_1.95O₄ powders prepared by MTO show higher specific capacity and better cycling performance than the one prepared by EMD.     

插层化合物LiV2O4的制备与实验研究

用化学方法从层状化合物LiVO₂中引出0.5个Li后得到Li_0.5VO₂,再经过低温真空热处理制备出尖晶石结构化合物LiV₂O₄,类似地处理Li_0.465VO₂,得到缺Li的Li_0.93V₂O₄,LiV₂O₄和Li_0.93V 关键词：     

六方相InGaN外延膜的显微Raman散射

用X射线衍射(XRD)技术和显微Raman散射方法对金属有机化学气相沉积(MOCVD)法生长的六方相In_xGa_1-xN薄膜样品进行了研究，观察到了相分离现象和LO声子-等离子耦合模(LPP⁺)，讨论了In_xGa_1-xN的A₁(LO)模被屏蔽的主要物理机制.同时，对Raman谱中E₂和A₁(TO)声子模进行了分析和讨论.在In_xGa_1-xN样品的低温Raman谱中还观察到单电子跃迁产生的Raman散射信号. 关键词： Raman散射 X射线衍射 相分离 应力 LO声子-等离子耦合     

Structural and magnetic phase transitions in (Chloroanilinium)2CuX4 (X = Cl, Br)

Successive structural phase transitions of (4-ClC₆H₄NH₃)₂CuCl₄, which occur in a very narrow temperature range were reinvestigated by Fourier transform nuclear quadrupole resonance (FT NQR) measurements. The phase transitions at 275.5 and 277.0 K were confirmed. The effect of the deuteration of the ammonium end on these transitions was studied. The³⁵Cl NQR frequencies of organic cation were observed to decrease by about 4 kHz and the phase transition temperatures to decrease by about 2 K by the deuteration, suggesting that the ?NH₃ ⁺ … Cl hydrogen bond is weakened by the deuteration. The magnetic phase transition temperature of 8.6 K showed no remarkable change within experimental error by the deuteration. It was found that the magnetically ordered state is broken by the radio-frequency magnetic field of about 15–35 Oe usually employed in pulsed NQR. However, in the deuterated compound (4-ClC₆H₄ND₃)₂CuCl₄, the ordered state was found to be stabler for the usual radiofrequency power. By combining with the NQR data of (4-ClC₆H₄NH₃)₂CuBr₄ and (3,5-Cl₂C₆H₃NH₃)₂CuCl₄, the possibility is discussed of tuning the interlayer interaction between the organic cation layer and the inorganic complex anion layer by the halogen substitution in the organic cation as well as by the halogen replacement in the inorganic complex anion.     

Rietveld refinement results on three nonstoichiometric monoclinic NASICONs

The results of three powder Rietveld refinements of monoclinic NASICONs, prepared by different methods, are examined. Neutron TOF data were collected on two samples: a sol-gel prepared NASICON was found to have the formula Na₃Zr_1.93Si₂PO_11.86 and a reheated commercially available NASICON a formula of Na_3.17Zr_1.93Si_1.9P_1.1O₁₂. Following our neutron study on a nonstoichiometric hydrothermally prepared NASICON we prepared the same nonstoichiometric phase by sol-gel methods and X-ray Rietveld analysis yielded the formula Na_3.2Zr_1.68Si_1.84P_1.16O_11.54. These stoichiometries can be represented by the general formula Na_1+4y+xZr_2−y−zSi_xO_12−2z where z represents the ZrO₂ mole deficiency and y the amount of Zr⁴⁺ vacancies compensated by 4Na⁺. These differences in stoichiometry are accompanied by structural differences such as Si/P segregation and variations in cavity occupancy by Na⁺. It is proposed that the method of preparation is largely responsible for the observed differences.     

The study of transition on NiFe2O4 nanoparticles prepared by co-precipitation/calcination

In this study, the NiFe₂O₄ nanoparticles have been prepared by co-precipitation and calcination process. Using a vibrating sample magnetometer (VSM), transmission electron microscopy (TEM), X-ray diffraction (XRD), energy dispersive spectrometer of X-ray (EDX), and X-ray photoelectron spectroscopy (XPS), the samples obtained by co-precipitation and then by further calcination have been analyzed. The experimental results show that the precursor synthesized by co-precipitation is the composite of both amorphous FeOOH and Ni(OH)₂, but has no amorphous NiFe₂O₄. The results of both EDX and XPS revealed that the FeOOH species is wrapped up by Ni(OH)₂ species. In the calcination process, the amorphous composite is dehydrated and transformed gradually into crystalline NiFe₂O₄ nanoparticles, with the metal ions diffusing. The reaction is different from the one used to prepare other ferrite (e.g., CoFe₂O₄, MnFe₂O₄, Fe₃O₄, etc.) nanoparticles directly by co-precipitation. With increasing calcination temperature, the NiFe₂O₄ grains grow and the magnetization is enhanced.     

Magnetic properties of core-shell catalyst nanoparticles for carbon nanotube growth

Two types of core-shell nanoparticles have been prepared by laser pyrolysis using Fe(CO)₅ and C₂H₂ or [(CH₃)₃Si]₂O as precursors and C₂H₄ as sensitizer. The first type (about 4 nm diameter) - produced by the decomposition of Fe(CO)₅ in the presence of C₂H₄ and C₂H₂ - consists of Fe cores protected by graphenic layers. The second type (mean particle size of about 14 nm) consists also of Fe cores, yet covered by few nm thick γ-Fe₂O₃/porous polycarbosiloxane shells resulted from the [(CH₃)₃Si]₂O decomposition and superficial oxidation after air exposure. The hysteresis loops suggest a room temperature superparamagnetic behavior of the Fe-C nanopowder and a weak ferromagnetic one for larger particles in the Fe-Fe₂O₃-polymer sample. Both types of nanoparticles were finally used as a catalyst for the carbon nanotube growth by seeding Si(100) substrates via drop-casting method. CNTs were grown by Hot-Filament Direct.Current PE CVD technique from C₂H₂ and H₂ at 980 K. It is suggested that the increased density and orientation degree observed for the multiwall nanotubes grown from Fe-Fe₂O₃-polymer nanoparticles could be due to their magnetic behavior and surface composition.     

Ga30Sb70/Sb80Te20纳米复合多层薄膜的相变特性研究

采用磁控二靶(Ga₃₀Sb₇₀和Sb₈₀Te₂₀)交替溅射方法制备了新型Ga₃₀Sb₇₀/Sb₈₀Te₂₀纳米复合多层薄膜, 对多层薄膜周期中Ga₃₀Sb₇₀层厚度对相变特性的影响进行了研究. 结果表明, 多层薄膜的结晶温度可以通过周期中Ga₃₀Sb₇₀层厚度进行调节, 且随着Ga₃₀Sb₇₀层厚度的增加而升高. Ga₃₀Sb₇₀/Sb₈₀Te₂₀纳米复合多层薄膜的光学带隙随Ga₃₀Sb₇₀层厚度的增加而增大. 采用皮秒激光脉冲抽运光探测技术研究了多层薄膜的瞬态结晶动力学过程, 利用不同能量密度的皮秒激光脉冲可以实现Ga₃₀Sb₇₀/Sb₈₀Te₂₀多层薄膜非晶态和晶态的可逆转变.     

Formation mechanisms and crystallographic characteristics of metastable VO2(A) nanofiber hydrothermally synthesised in V2O5–H2C2O4–H2O system

There are many similarities between VO₂(B) and VO₂(A) from crystallographic view. However, missing of VO₂(A) during the preparation of VO₂ polymorph confused many researchers. Here, the preparation of VO₂(A) was studied systemically via a hydrothermal method in V₂O₅–H₂C₂O₄–H₂O system. As a metastable phase, it can be transferred from VO₂(B) by assembling process. Usually, poly-crystal VO₂(A) nano-fibers are formed by this process. On contrast, owing to the small energy gap between meta-stable VO₂(A) and stable VO₂(R), single crystal VO₂(A) with regular shape can also be obtained by exfoliating some parts of VO₂(R) during non-equilibrium cooling process. VO₂(A) has higher phase transition temperature than stable VO₂(R). The hysteresis in this phase transition can be observed by DSC measurement and the phase transition temperature of VO₂(A) can be tuned down by tungsten doping.     

ATP synthase: from single molecule to human bioenergetics

ATP synthase (F_oF₁) consists of an ATP-driven motor (F₁) and a H⁺-driven motor (F_o), which rotate in opposite directions. F_oF₁ reconstituted into a lipid membrane is capable of ATP synthesis driven by H⁺ flux. As the basic structures of F₁ (α₃β₃γδε) and F_o (ab₂c₁₀) are ubiquitous, stable thermophilic F_oF₁ (TF_oF₁) has been used to elucidate molecular mechanisms, while human F₁F_o (HF₁F_o) has been used to study biomedical significance. Among F₁s, only thermophilic F₁ (TF₁) can be analyzed simultaneously by reconstitution, crystallography, mutagenesis and nanotechnology for torque-driven ATP synthesis using elastic coupling mechanisms. In contrast to the single operon of TF_oF₁, HF_oF₁ is encoded by both nuclear DNA with introns and mitochondrial DNA. The regulatory mechanism, tissue specificity and physiopathology of HF_oF₁ were elucidated by proteomics, RNA interference, cytoplasts and transgenic mice. The ATP synthesized daily by HF_oF₁ is in the order of tens of kilograms, and is primarily controlled by the brain in response to fluctuations in activity.     

50—5000 eV电子被C4H8O,C5H10O2, C6H5CH3和C4H8O2散射的总截面

使用电子被C, H和O原子散射总截面的实验数据, 利用修正后的可加性规则计算了能量为50—5000eV的电子被4个复杂大分子C₄H₈O, C₅H₁₀O₂, C₆H₅CH₃和C₄H₈O₂散射的总截面, 并将计算结果与实验结果及其他理论计算结果进行了比较. 结果表明, 即 关键词： 电子散射 可加性规则 总截面 几何屏蔽效应     

磁控溅射法制备二氧化钒薄膜最佳参量的研究

用X射线电子能谱仪(XPS)对不同条件下用磁控溅射法制备的VO₂薄膜进行测试,得到VO₂薄膜内部组成成份的信息.研究了获得高含量VO₂薄膜的最佳制备参量.同时还观察到V₂O₃、VO₂、V₂O₅以接近含量共存的现象,这与以前研究所给出的薄膜几乎只由V₂O₃、VO₂、V₂O₅中的两种组成的结论有所不同.     

Variation of magnetic state of amorphous Fe90Zr10 and Fe91Hf9 by the charge of hydrogen

Amorphous Fe₉₀Zr₁₀ and Fe₉₁Hf₉ ribbons were charged with hydrogen by the electrochemical method up to Fe₉₀Zr₁₀H₂₆ and Fe₉₁Hf₉H₁₅, respectively, and the change in magnetic structures were analyzed by Mössbauer spectrometry. The internal magnetic field appeared by the charge of hydrogen, the degree of change being depended on amounts of hydrogen included in amorphous Fe₉₀Zr₁₀ and Fe₉₁Hf₉, although Fe₉₁Hf₉ absorbed hydrogen more slowly than Fe₉₀Zr₁₀. The differences of hydrogen inclusion and Mössbauer hyperfine structure between Fe₉₀Zr₁₀ and Fe₉₁Hf₉ were discussed based on the results of a hyperfine field distribution and the radial distribution functions of Fe?Fe obtained by EXAFS.     

Valence control of cobalt oxide thin films by annealing atmosphere

The cobalt oxide (CoO and Co₃O₄) thin films were successfully prepared using a spin-coating technique by a chemical solution method with CH₃OCH₂CH₂OH and Co(NO₃)₂·6H₂O as starting materials. The grayish cobalt oxide films had uniform crystalline grains with less than 50 nm in diameter. The phase structure is able to tailor by controlling the annealing atmosphere and temperature, in which Co₃O₄ thin film was obtained by annealing in air at 300-600, and N₂ at 300, and transferred to CoO thin film by raising annealing temperature in N₂. The fitted X-ray photoelectron spectroscopy (XPS) spectra of the Co2p electrons are distinguishable from different valence states of cobalt oxide especially for their satellite structure. The valence control of cobalt oxide thin films by annealing atmosphere contributes to the tailored optical absorption property.     

Reactions at the interface La0.5Ca0.5MnO3-YSZ/Al2O3 under anodic current

The reaction at the interface of a solid electrolyte cell between air electrode (La_0.5Ca_0.5MnO₃) and YSZ-electrolyte with different Al₂O₃-contents was investigated by electron microscopy (SEM) and x-ray diffraction (XRD). Formation of MnAl₂O₄ was detected in a 5 μm diffusion zone within the electrolyte. MnAl₂O₄ formation can be explained by diffusion of Mn-ions into the electrolyte and subsequent reaction with the α-Al₂O₃ grains during sintering. Cell performance and long-term stability in SOFC operation are not negatively affected by MnAl₂O₄ formation. However a rise in electrode resistance and slow delamination of perovskite oxide electrode were observed after some hours of electrolysis. This reaction is the consequence of oxygen gas pressure at the electrolyte in the MnAl₂O₄ diffusion zone. It is caused by local increase of electronic conductivity by MnAl₂O₄ formation. Long-term stability also for electrolysis conditions has been achieved by an additional intermediate YSZ-layer between air electrode and electrolyte. Paper presented at the 3rd Euroconference on Solid State Ionics, Teulada, Sardinia, Italy, Sept. 15–22, 1996     

Electron tunneling into thin films of Y1Ba2Cu3O7

We have fabricated tunnel junctions on thin films of Y₁Ba₂Cu₃O₇ which were epitaxially grown by magnetron sputtering on (100) and on (110) oriented SrTiO₃ substrates. These junctions of the type Y₁Ba₂Cu₃O₇/barrier/Pb or In showed with high reproducibility in the conductance a gap-like structure with the maxima near±16mV. We supplied experimental arguments that this structure reflects properties of the quasi particle excitation spectrum of Y₁Ba₂Cu₃O₇. The gap-like structure was found to disappear atT _c mainly by weakening and not by a shift of the peaks to lower voltages.     

He-Ne激光选育高木质素降解率的白腐真菌Lx

用He-Ne激光对一株木质素降解活性较高的白腐真菌L₁进行选育.将该菌的菌丝体和原生质体多次照射诱变,结果得出:在波长632.5nm,用功率为6mW和7mW照射该菌的菌丝体,选育出的菌株L₆和L₇木质素降解率可达38.1%和39.88%,比出发菌株L₁提高了33%和39%.用功率9mW的He-Ne激光辐照原生质体,照射20min时,原生质体致死率已达100%.在照射时间为10min时,选育出一株木质素降解率达43.03%的菌株L_x,比出发菌株L₁提高了50%.同工酶分析显示该菌株发生了稳定的遗传突变.     

Introducing CdS into two- and three-dimensional photonic crystals

SiO₂/air three-dimensional (3D) periodic structures were fabricated by removing Si layers partially from Si/SiO₂ 3D photonic crystals (PhCs) formed by using autocloning. CdS/SiO₂ 3D periodic structures were formed by introducing CdS into the SiO₂/air structures by the TEA method and photoluminescence (PL) was observed from the introduced CdS. TiO₂/air/CdS two-dimensional (2D) PhCs were also fabricated by introducing CdS into the voids of TiO₂/air 2D periodic structures, in which SiO₂ layers were partially etched out from TiO₂/SiO₂ 2D PhCs fabricated by using autocloning. PL radiating normal to the surface was measured and large polarization dependence was observed.     

Phase transition characteristics of Ge–Sb–Te pseudobinary alloys in laser irradiation measurement

Optical switching and structural transformation of GeTe–Sb₂Te₃ pseudobinary alloys, Ge₂Sb₂Te₅, Ge₁Sb₂Te₄, and Ge₁Sb₄Te₇, were studied for data storage application. As-deposited Ge₂Sb₂Te₅, Ge₁Sb₂Te₄, and Ge₁Sb₄Te₇ thin films were amorphous and they crystallized to FCC and HCP upon heat treatment. Crystallization was accelerated by increasing the proportion of Sb₂Te₃ rather than GeTe in Ge–Sb–Te compounds; this was observed by reflectivity changes under nanosecond laser irradiation in static tester. The different crystallization kinetics according to composition might be affected by the structural incompatibility of GeTe under the ‘Umbrella Flip’ theory.     

ac ionic conductivity of hollandite type compounds from 100 Hz to 37.0 GHz

The frequency- and temperature-dependences of a.c. ionic conductivity of one-dimensional super-ionic conductors K-priderites with a hollandite type structures were investigated from 100 Hz to 37.0 GHz. Four kinds of K-priderite, K_1.6Mg_0.8Ti_7.2O₁₆, (K_1.3, Li_0.1) Mg_0.7Ti_7.3O₁₆, K_1.6Al_1.6Ti_6.4O₁₆ and (K_1.3, Li_0.2) Al_1.5Ti_6.5O₁₆, were studied. An equivalent circuit to combine the data of the complex conductivity at low and high frequencies was proposed. The data of complex conductivity at low frequencies can be analyzed in terms of the moving box model proposed by Beyeler et al. The transport of K⁺ ions at low frequencies is characterized by the cooperative motion of the K⁺ ions with various mobilities and is accompanied with the polarization of the K⁺ ions in the channels. The ion transport across intrinsic barriers at or above microwave frequencies is characterized by the frequency-independent ionic conductivity and is interpreted by the configurational model proposed by Beyeler et al. The height of intrinsic barriers is related to the lattice constants of a crystal.