High-pressure synthesis and local structure of corundum-type In(2-2x)Zn(x)Sn(x)O(3) (x ≤ 0.7)

The corundum-type In(2-2x)Zn(x)Sn(x)O(3) solid solution (cor-ZITO, x ≤ 0.7) was synthesized at 1000 °C under a high pressure of 70 kbar. cor-ZITO is a high-pressure polymorph of the transparent conducting oxide bixbyite-In(2-2x)Zn(x)Sn(x)O(3) (x ≤ 0.4). Analysis of the extended X-ray absorption fine structure suggests that significant face-sharing of Zn and Sn octahedra occurs, as expected for the corundum structure type. In contrast to the ideal corundum structure, however, Zn and Sn are displaced and form oxygen bonds with lengths that are similar to those observed in high-pressure ZnSnO(3). Powder X-ray diffraction patterns of cor-ZITO showed the expected unit cell contraction with increased cosubstitution, but no evidence for ilmenite-type ordering of the substituted Zn and Sn. A qualitative second harmonic generation measurement, for the solid solution x = 0.6 and using 1064 nm radiation, showed that Zn and Sn adopt a polar LiNbO(3)-type arrangement.     

Determination of different local potentials of zero charge of a Pd–Au(111) heterogeneous surface

Local values of potential of zero charge (pzc) and potential of zero total charge (pztc) have been determined for Au(111) surfaces partially covered with palladium at low coverages. The pztc of the palladium islands has been measured with the CO charge displacement procedure. The adsorption of CO only takes place on the palladium-covered domains allowing us to selectively displace the charge residing in this part of the surface. The resulting pztc values of the palladium islands are located around 0.25 V for the entire range of palladium coverages. The pzc of gold-uncovered areas has been determined by identifying the position of the differential capacity minimum (0.52 V). It appears that this pzc is only slightly affected by the presence of deposited palladium.     

On the single-electron local kinetic energy

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Investigating the local structure of B-site cations in (1-x)BaTiO3–xBiScO3 and (1-x)PbTiO3–xBiScO3 using X-ray absorption spectroscopy

The structural properties of (1-x)BaTiO₃–xBiScO₃ and (1-x)PbTiO₃–xBiScO₃ were investigated using powder X-ray diffraction and X-ray absorption spectroscopy. Diffraction measurements confirmed that substituting small amounts of BiScO₃ into BaTiO₃ initially stabilizes a cubic phase at x = 0.2 before impurity phases begin to form at x = 0.5. BiScO₃ substitution also resulted in noticeable changes in the local coordination environment of Ti⁴⁺. X-ray absorption near-edge spectroscopy (XANES) analysis showed that replacing Ti⁴⁺ with Sc³⁺ results in an increase in the off-centre displacement of Ti⁴⁺ cations. Surprisingly, BiScO₃ substitution has no effect on the displacement of the Ti⁴⁺ cation in the (1-x)PbTiO₃–xBiScO₃ solid solution.     

A local spin evaluation into the active site models of [2Fe2S] ferrodoxin [Fe_2S_2(SR)_4]~(2-) (R=-H, -CH_3)

To test the feasibility of local spin theory of Davidson and Clark for ferrodoxin clusters, the models [Fe2S2(SR)4]2- (R=-H, -CH3) are chosen for evaluation. This purpose is realized by calculating the local spin expectation values , , and mA and discussing the connection between these expected values and the Heisenberg spin model (HSM) and the Noodleman broken-symmetry approach. In practical calculation, the spin-unrestricted Hartree-Fock (UHF) and spin-polarized density functional theory (DFT) are used and the calculational qualities of these two methods are also discussed. In addition, the theoretical magnetic coupling constants JAB of these models are calculated by various computational schemes for comparison with both theoretical and experimental results previously reported.     

Li_(3.22)Na_(0.569)Mn_(5.78)O_(12.0)的电化学性能

以L iOH.H2O和Mn(CH3COO)2.2H2O作原料,应用微波-固相两段烧结法合成具有L i4Mn5O12结构特征,组成为L i3.22Na0.569Mn5.78O12.0的锂离子电池正极材料.XRD分析表明,在380℃的后处理温度下,微波烧结前处理有利于生成纯L i4Mn5O12尖晶石相.充放电实验表明,在4.5~2.5V电压区间,新制样品的初始放电容量为132 mAh.g-1,100循环的容量衰减率为6.8%;4个月存放样的初始放电容量为122 mAh.g-1,100循环的容量衰减率为17.4%.表现出较好的充放电性能和循环寿命.微波烧结使样品的Mn-O键被加强.     

Ce_(0.8)Nd_(0.2)O_(1.9)-La_(0.95)Sr_(0.05)Ga_(0.9)Mg_(0.1)O_(3-δ)固体复合电解质的结构和电性能

采用溶胶-凝胶法分别制备La0.95Sr0.05Ga0.9Mg0.1O3-δ(LSGM)和Ce0.8Nd0.2O1.9(NDC)电解质,并在NDC溶胶中加入0-15%(w,质量分数)的LSGM预烧粉体制得NDC-LSGM复合电解质,研究不同质量比复合电解质的结构和电性能.采用X射线衍射(XRD)、场发射扫描电子显微镜(FE-SEM)和X能量色散谱仪(EDS)对样品进行结构表征,交流(AC)阻抗谱测试样品导电性能.结果表明:NDC-LSGM复合体系主要由立方萤石结构相、钙钛矿结构相和杂质相组成;LSGM的添加可促进晶粒的生长,产生大量相界面,清除或降低SiO2有害影响,明显提高晶界导电性;LSGM质量分数为10%的样品NL10具有最高晶界电导率和总电导率,400°C时NL10的晶界电导率σgb和总电导率σt分别为12.15×10-4和3.49×10-4S cm-1,与NDC的σgb(1.41×10-4S cm-1)和σt(1.20×10-4S cm-1)相比分别提高了7.62和1.91倍,总电导率的提高主要归因于晶界电导率的影响.     

La_(0.7)Pr_(0.15)Nd_(0.05)Mg_(0.3)Ni_(3.3-x)Co_(0.2)Al_(0.1)(Co_(0.75)Mn_(0.25))_x(x=0.0,0.2,0.4,0.6)的电化学性能研究

在Ar气保护下用悬浮熔炼制备La0.7Pr0.15Nd0.05Mg0.3N i3.3-xCo0.2A l0.1(Co0.75Mn0.25)x(x=0.0,0.2,0.4,0.6)合金,系统研究了Co和Mn对合金储氢性能和电化学性能的影响。XRD相分析表明,合金相主要由(La,Pr)(N i,Co)5,LaMg2N i9,(La,Nd)2N i7和LaN i3相组成;添加Co和Mn后合金中(La,Pr)(N i,Co)5,(La,Nd)2N i7和LaN i3相晶胞体积增加,LaMg2N i9相晶胞体积变小。合金放氢PCT曲线测试表明,随着合金中Co和Mn含量的增加,合金吸氢量先减小后增加,放氢平台压下降,合金氢化物稳定性增加。合金电极电化学性能测试表明,添加Co和Mn使合金电极放电容量减小,容量保持率S100从53.2%(x=0.0)增加到63.0%(x=0.6),合金电极的电循环稳定性增强,高倍率放电性能HRD1500先增加后减小。此外,合金电极的极化电阻先减小后增加,交换电流密度、循环伏安特性阳极峰电流密度和极限电流密度先增加后减小,合金内氢原子扩散系数先增加后减小,表明添加适量的Co和Mn可以提高合金电...     

Synthesis and Crystal Structure of Trans-diaquabis(hexamethylenetetramine-N)bis(isothiocyanato)cobalt(Ⅱ) trans-tetraaquabis(isothiocyanato)cobalt(Ⅱ) dihydrate

1 INTRODUCTION Supramolecular compounds assembled by coordination covalent bonding or hydrogen bonding are of considerable interest due to their potential applications in developing new materials with magnetic, optical and catalytic properties[1]. One of the synthesis methods used to construct the functional compounds is that octahedral metal ion connects to polydentate ligand such as 4, 4?bipyridine, pyrazine and so on to form multi-dimensional supramolecular polymer[2]. Hmt (hexamethyl…     

Novel Ba_(0.5)Sr_(0.5)Fe_(0.8)Zn_(0.2)O_(3-δ) membranes for POM

A novel cobalt-free perovskite based on Ba_(0.5)Sr_(0.5)Fe_(0.8)Zn_(0.2)O_(3-δ)(BSFZ)were prepared by EDTA-citric acid method.The lattice constants of the BSFZ perovskite were characterized by in situ high-temperature X-ray diffraction(HTXRD).The thermal expansion coefficient of BSFZ is 10.5×10~(-6)K~(-1),which is lower than that of cobalt-based perovskite materials.The BSFZ membrane was also used to construct reactors for the partial oxidation of methane(POM)to syngas.Results show that the BSFZ membrane...     

双水相萃取法分离铍(Ⅱ)、铁(Ⅲ)与铁(Ⅱ)、铬(Ⅲ)、锰(Ⅱ)、铝(Ⅲ)

研究了在聚乙二醇2000(PEG)-硫酸钠(Na2SO4)-邻苯二酚紫(PV)体系中铍(Ⅱ)、铁(Ⅲ)、铁(Ⅱ)、铝(Ⅲ)、铬(Ⅲ)、锰(Ⅱ)的萃取行为。试验结果表明,铍(Ⅱ)在pH 3.5-7.0及铁(Ⅲ)在pH 4.0-7.0范围内可以被PEG相几乎完全萃取,而铝(Ⅲ)、铬(Ⅲ)在pH 1.0-7.0、锰(Ⅱ)在pH 1.0-4.5、铁(Ⅱ)在pH 1.0-4.5则不被萃取。从而实现了将铍(Ⅱ)(pH 3.5)、铁(Ⅲ)(pH 5.0)与铝(Ⅲ)、铬(Ⅲ)、锰(Ⅱ)、铁(Ⅱ)混合离子的定量分离。同时探讨了PEG相的萃取机理。     

X-ray structures of trans-dichloro(4-methylpyrimidine) (η1-phenyl)bis(pyridine)rhodium(III) hydrate and trans-dichloro(phenyl)tris(triphenylstibine)rhodium(III) ethylacetate solvate. Molecular orbital analysis of trans-dichloro (4-methylpyrimidine)(η1-phenyl)bis(pyridine)rhodium(III)

The crystal and molecular structure of trans-dichloro(4-methylpyrimidine)(η ¹ -phenyl)cis-bis(pyridine)rhodium(III) water solvate, 1x 0.17H₂ O, and trans-dichloro(η ¹ -phenyl)tris(triphenylstibine)rhodium(III) ethylacetate solvate, 2x CH₃ CO₂ CH₂ CH₃ have been studied via X-ray diffraction from a single crystal at room temperature. The final refinement converged to R1 conventional index of 0.0350 and 0.0361 for the structural analysis of 1x 0.17H₂ O [space group R(-3) and 2x CH₃ CO₂ CH₂ CH₃ P(-1) , respectively. The 4-methylpyrimidine ligand (Pym) is only weakly bound to Rh in 1, as shown by the long Rh-N distance (2.251(4) Å), compared to the Rh N(pyridine) lengths average, 2.066(4) . N-C bond distances involving the N donor average 1.329(6) and 1.345(6) for Pym and pyridine (Py) ligands, respectively. The C N C bond angle on the donor is 114.1(5)° for Pym and average 117.4(4)^° for Py.The structure of the complex molecule of 2x CH₃ CO₂ CH₂ CH₃ has some differences when compared to that of the corresponding acetone solvate previously studied in this laboratory (Cini, R., Giorgi, G. and Pasquini, L., Inor`. Chim. Acta, 1992, 196, 7). The two structures differ mainly by the orientation of the phenyl donor with respect to the Cl-Rh-Cl axis (which is more eclipsed for the ethylacetate solvate) and by the conformation of the SbPh₃ ligands.Density functional calculations at the B3LYP/LANL2DZ level with full geometry optimization were carried out on the free Pym molecule and on some Sc(N ¹ Pym) ^{3 +}and Sc(N ² Pym) ^{3 +} model molecules. The effect of metal coordination consists mainly in enlarging the (Sc)N-C bond distances up to 0.150Å, whereas the C-N(Sc)-C bond angle decreases of 1.9°. Significant changes on other bond lengths and angles relevant to ring atoms of Pym occur upon metal coordination to the nitrogen atom. The metal coordination to N(2) is less favorable than to N(1) of 7.5 kcal for 1:1 species of Sc^{3 +}Extended Hückel calculations showed that HOMO consists mostly of metal-d orbitals with some character of chloride and phenyl and pyrimidine ligands, whereas LUMO is composed of phenyl, pyridine and pyrimidine orbitals. The method well reproduces the Rh-N and Rh-C bonding distances and gives Rh-C dissociation energy 2.38 and 5.48 times that for the Rh-N(Py) and Rh-N(Pym) bonds, respectively.     

Nd_2(Fe_(1-x)Co_x)_(14)B和Y_2(Fe_(1-x)Co_x)_(14)B的磁性

用磁测量和X-射线衍射研究了Nd_2(Fe_(1-x)Cox)_(14)B和Y_2(Fe_(1-x)Cox)_(14)B的晶格结构和内禀磁性。结果表明,低温下当钴含量较少时,Y_2(Fe_(1x)Cox)_(14)B的磁晶格向异性随钴含量的增加而增加,在1.5K和150K温度下,分别在x为0.4和0.2左右时磁晶各向异性常数达到极大;室温时的磁晶各向异性常数却随钴含量的增加而单调下降。用钴代换铁,对Nd_2(Fe_(1-x)Cox)_(14)B的自旋再取向温度的影响是复杂的。1.5K的饱和磁化强度在x=0.1左右达到极大。钴可以显著提高居里温度,对于Nd_2(Fe_(1-x)Cox)_(14)B和Y_2(Fe_(1-x)Cox)_(14)B,钴的作用几乎相同,表明居里温度主要由3d过渡金属原子之间的交换作用决定。     

New access to (η(5)-cyclohexadienyl)Mn(CO)3 and cationic (η(6)-arene)Mn(CO)3 complexes by Suzuki-Miyaura reaction

First Suzuki-Miyaura coupling reactions applied to (η(5)-chloro-cyclohexadienyl)Mn(CO)3 complexes are described and lead to the syntheses of (η(5)-aryl-cyclohexadienyl)Mn(CO)3 and of cationic (η(6)-arene)Mn(CO)3 complexes after rearomatization. The structures of two of the new complexes have been investigated by X-ray diffraction study.     

Does an exact local exchange potential exist?

In Kohn–Sham density functional theory, equations for occupied orbital functions of a model state are derived from the exact ground‐state energy functional of Hohenberg and Kohn. The exchange‐correlation potential in these exact Kohn–Sham equations is commonly assumed to be a local potential function rather than a more general linear operator. This assumption is tested and shown to fail for the exchange potential in a Hartree–Fock model for atoms, for which accurate solutions are known. This revised version was published online in July 2006 with corrections to the Cover Date.     

~(13)C核磁共振(六)

分子式为C_6H_8O的哪一个化合物与图E-11符合? 取谱条件: 溶剂:CDCl_3(δ77.2三重峰) 浓度:50V/V％温度:28℃测定频率:22.63MHz 去偶:上——~1H偏共振去偶(500次) 下——~1H宽带去偶(100次) [解答]C_6H_8O含有三个双键当量。在~(13)C谱中找到一个羰基(δ198.65)以及一个C=C键(δ150.6及129.85)。还余下一个双键与三个次甲基(δ38.2,25.75及22.95)。总结起     

~(13)C核磁共振(五)

习题1 分子式为C_4H_(10)S的哪一个化合物符合图E-1的~(13)C谱?对此谱作出归属。取谱条件: 溶剂:CDCl_3(δ77.25处有三重峰,图中未画出) 浓度:50V/V％温度:28℃测定频率:22.63MHz 去偶:上——~1H偏共振去偶(200次) 下——~1H宽带去偶(100次)     

~(13)C核磁共振(七)

习题16 1,3,5-三硝基苯与丙酮在氢氧化钾的乙醇溶液存在下反应生成一种蓝紫色的Meisenheimer钾盐,见谱E-16。分析此谱并给出从谱所得最重要的论点以支持此盐的结构。取谱条件: 溶剂,(eD,),50(3,.7七重峰,Je-一20.5Hz) 浓度:饱和溶液温度:28℃测定频率:22.63 MHz 去偶.上.偶合谱(25000次),附有放大四倍的部分谱下:几H宽带去偶( 5000次)〔解答〕谱的归属     

~(13)C核磁共振(四)

9 ~(13)C自旋-晶格弛豫时间(T_1)的测量及应用 9.1 测定T_1的方法 9.1.1 倒向—恢复法此法是用(180°-τ-90°)_n脉冲系列作用于样品。磁化矢量M_0在180°脉冲作用下倒向(图20b),在自旋-晶格弛豫过程中,磁化矢量从-M_0经0到 M_0弛豫,在这一过程中,即过了时间τ后,90°脉冲将部份弛豫的磁化矢量M_τ旋转到X(?)Y平面中,并在接收线圈中感应出FID信号。如果τ很短,M_τ还是负的(M_τ<0),90°脉冲(?)_1,作用后M_τ沿X向负Y轴旋转(图20c),     

~(13)C核磁共振(三)

8.1 通过一个键的C与H偶合除了化学位移之外,C—H的偶合常数也能提供重要的信息,测量J值时必须取不去偶或用交替脉冲双共振方法。这两种方法都需时较长,并且要求样品量较多。~1J_(CH)也可从~1H谱的~(13)C卫星线测得。 ~1J_(CH)在120-130Hz之间~2J(CH)、~3J(CH)~4J(CH)都小于