RESr2RuCu2O8(RE=Gd和Eu)的合成与物性研究

报道了磁性超导体RESr2RuCu2O8(RE=Gd和Eu)单相样品的合成以及对其结构和物性的研究。结果表明，这类化合物的结构和YBa2Cu3O7-δ相类似；在这两类化合物中，超导电性与弱铁磁有序共存；两样品铁磁相变温度TM分别为136，130K，超导临界温度TC分别为46，35K；由于Gd^3 和Eu^3 离子磁矩的不同，两样品的磁性质存在一定的差别。     

LaMg_2Cu_(1-x)Ni_x(x=0～0.90)合金的相结构及储氢性能

利用真空感应熔炼技术制备了LaMg2Cu1-xNix(x=0,0.10,0.25,0.50,0.75,0.90)合金,并在0.06MPa氩气保护下于723K退火6h得到测试所用合金铸锭。XRD表明合金LaMg2Cu1-xNix含有ThCr2Si2型的LaMg2Cu2相和CeMg3型的LaMg3相以及少量未知相,随着x的增加,LaMg2Cu2相的晶胞体积先增加后减小,而LaMg3相的晶胞体积几乎不变。通过SEM观察,发现Ni可以有效的减小合金在吸放氢过程中的粉化。当x0.50时,Ni对合金的吸氢速率降低;而当x≥0.50时,Ni的加入可以极大的提高合金的吸氢速率,合金在50s左右就能达到最大吸氢量的90%。当x=0.50时,合金具有较好的综合储氢性能,合金在473K下吸氢量为3.741wt%,49s就可达到最大吸氢量的90%以上。     

MmB5贮氢合金的结构和性能

近十年未对AB5型合金的研究表明，某些多元取代的LaNi5基合金可作为MH／Ni电池的负极材料，且具有容量大，寿命长等优点[1，2]．LaNi5虽然具有吸放氢量较大、平台氢压平整和压力滞后小等优良性能，但不耐硷腐蚀、吸氢后易粉化，其氢化物的分解氢压较高，故不能作为负板材料．以Co部分地取代Ni可有效地降低氢化物的分解氢压·混合稀土（Mm）取代La，虽容量有所下降，但从原料成本上看是有益的．本工作试图从MmB5多元合金晶体结构的研究，来探讨Mm中La和Ce的相对含量对吸放氢性能和电化学容量的影响．1实验Mllin。合金样品由金属Ni，…     

SiO_2基底中MnFe_2O_4纳米晶的制备与表征

在N,N-二甲基甲酰胺(DMF)存在下,以溶胶-凝胶技术成功地制备了无定形二氧化硅基底中均匀分布的MnFe_2O_4纳米晶.由粉末X射线衍射和电子衍射确证了MnFe_2O_4纯相的生成. 由粉末X射线衍射和红外吸收光谱研究了MnFe_2O_4纳米晶形成过程.尖晶石结构的MnFe_2O_4在800℃时开始形成,900℃时基本完成.磁性质测量表明在烧结到900℃的样品中,MnFe_2O_4纳米晶室温具有超顺磁性,78K时为软磁性.1000℃ 和1100℃下得到的样品室温和78K时都具有软磁性.     

Tb(Co_(1-x)Sn_x)_2合金的结构和磁热效应

通过X射线衍射和磁性测量研究了Tb(Co1-xSnx)2(x=0,0.025,0.050,0.075,0.100)合金的相结构和磁热性能。经分析可知Sn在TbCo2中的替代是有限的,X粉末衍射分析确定TbCo2具有MgCu2结构,其他样品由TbCo2,TbCo3和Tb5Sn3三相组成,TbCo2为主要相。随着Sn成分的增加,杂质相TbCo3和Tb5Sn3的含量增加,所有样品保持第二序磁相变。Sn的替代使磁相变的温度稍微有所提高,样品TbCo2的TC值为230 K,样品Tb(Co0.950Sn0.050)2的TC值为233 K,但Sn的成分继续增加,样品的TC值有所下降。在外加磁场2 T的作用下,样品Tb(Co1-xSnx)2(x=0,0.025,0.050,0.075)最大磁熵变值分别为3.44,2.29,1.64,1.16 J.kg-1.K-1。     

尖晶石结构MFe_2O_4(M=Ca,Mg,Cu,Zn)纳米晶粉末的制备和磁性能（英文）

采用新型氨基凝胶自燃法成功制备出尖晶石结构MFe_2O_4(M=Ca,Mg,Cu,Zn)纳米晶粉末。对合成粉体样品的物相、形貌和磁性能进行了详细的研究。经能量色散X射线谱分析确定了合成MFe_2O_4粉末的高纯度。系统地研究了所合成的MFe_2O_4纳米晶粉末的磁性能。所有样品的磁滞回线均较窄,表明了它们具有软磁的特征。经测试得出4种铁氧体的饱和磁化强度(M_s)分别为2.1,29.3,24.1和4.2 emu·g~(-1);剩余磁化强度(M_r)分别为0.2,2.3,11.4和0.2 emu·g~(-1)。这4种铁氧体样品的M_r/M_s值均小于0.5。对CaFe_2O_4和MgFe_2O_4两种典型铁氧体的零场冷却和场冷磁性能作了详细的研究。其中CaFe_2O_4样品的磁化强度在75 K以下有不一致的变化趋势,这是由于其发生了磁相变。     

Mg-20%(RE-Ni)(RE=La,Y,Mm)复合材料储放氢性能研究

通过磁悬浮熔炼和反应球磨相结合的方法成功制备出Mg-20wt%(RE-Ni)(RE=La,Y,Mm)复合储氢材料,主要研究了材料的物相结构和储放氢性能.结果表明.Mg-20wt%(RE-Ni)(RE=La,Y,Mm)复合储氢材料,具有相似的物相结构和吸放氢热力学性能,吸氢相均为MgH2和Mg2Ni,在同一温度下,合金只有一个放氢平台,表明两相具有良好的协同放氢效应.在复合体系中,Mg-20wt%(Y-Ni)具有最佳的综合储氢性能,表明Y具有最佳的催化效果,其在293 K,3.0 MPa H2,10 min的吸氢量和573 K,对0.1 MPa,15 min的放氢量可分别达到3.92%和4.75%,实现了室温快速大量吸氢和较温和条件下的快速放氢.     

金属镱高压吸氘性能研究

大部分稀土金属与氢反应 ,都能很容易地生成三氢化物。但镱和铕却是例外 ,镱在氘压力小于 1 .0 3× 1 0 5Ｐａ时只生成二氘化物。文献报道金属镱在氢压力约为 2 .0ＭＰａ时生成ＹｂＨ2 .58,2 0 0～30 0℃等温线平台区从约ＹｂＨ2 扩展到接近ＹｂＨ2 .5,表明有两种不同的氢化物物相存在。基于ｖａｎ’ｔＨｏｆｆ计算得到ＹｂＨ2 .5(至二氢化物 )离解热约为 1 3.8ｋＪ/ｍｏｌＨ2 。对于在压力大于 0 .1ＭＰａ条件下获得的高含氢量氢化镱 ,Ｈａｒｄｃａｓｔｌｅ报道有一个ａ为 5 .1 92 的ｆｃｃ相与低氢含量的氢化物相共存[1 ] ,两个物相的存…     

LSDA+U方法研究Ni掺杂CuO和Cu掺杂NiO的电子结构和反铁磁学性质

光催化分解水制H2和光催化还原CO2是解决能源危机和全球变暖的有效途径.但是,由于粉末光催化剂存在回收效率低的问题,因而光催化成本很高.而磁性光催化剂便于回收和重复利用,因此人们把目光转向具有磁性的非光催化剂材料,试图通过改性使得磁性材料具有合适的水分解或者还原CO2的氧化还原电位.同时,对具有光催化活性但是没有磁性的材料进行磁化改性可以得到新型的磁性光催化剂.本文通过对本身具有磁性的NiO材料进行Cu掺杂能带调整,使调整后的NiO具有合适的氧化还原电位;对本身具有良好光催化氧化还原电位的CuO材料进行Ni掺杂磁化调整,使磁化后的CuO既有良好的氧化还原电位又有磁性.最终两种材料经过掺杂变成磁性光催化材料,既有较好的光催化性能,又可高效回收,因此有望在光催化领域具有潜在的应用前景.LSDA(局域自旋密度近似)+U(有效库仑相关能)计算方法能够很好地给出磁矩和禁带宽度等电子结构性质.本文通过LSDA+U计算方法对具有磁性的宽禁带半导体材料NiO进行电子结构改性研究,希望通过降低其禁带宽度、调整其氧化还原电位使之对太阳光有响应.因其同时具有磁性便于回收,使得光催化分解水制H2和光催化还原CO2成本高的问题得到解决.对NiO的磁胞进行了Cu掺杂计算,结果发现Cu的掺杂几乎没有引起NiO空间结构的变化,这是因为Cu和Ni的离子半径相近.通过对电子结构的计算发现掺杂体系的禁带变窄,并且在禁带中间出现了两条杂质能级,该杂质能级是由掺杂原子Cu 3d态组成.杂质能级的出现能够降低光生载流子在带隙中的复合,从而提高光催化效率.计算结果同时表明,Cu掺杂的NiO系统具有一个1μB的净磁矩,即Cu的掺杂使得NiO显示出磁性,而Ni的磁矩在掺杂前后几乎保持不变,由纯相的1.67μB增加到掺杂体系中的1.70μB.由于CuO本身低指数(111)面和(011)面具有合适的分解水制H2和还原CO2的氧化还原电位,如果对CuO进行磁化改性,可以使光催化剂CuO同时带有磁性,便于回收再利用.本文对CuO磁胞进行了Ni的掺杂计算.结果表明,由于离子半径相近,Ni掺杂几乎没有引起CuO空间结构的变化.掺杂后的体系具有一个1.66μB的净磁矩,同时Ni的掺杂引起多个杂质能级出现,靠近价带的杂质能级由Cu 3d态组成,而在导带底位置出现的杂质能级主要由Ni 3d态组成.整个能带向高能级方向平移.     

氢化燃烧法合成La2-xNixMg17(x=0.5,1,1.5)材料的储氢性能

采用氢化燃烧法制备La2-xNixMg17(x=0.5, 1, 1.5)三元体系储氢材料, 对其热力学、动力学进行研究发现: 该体系材料具有很好的活性和较高的储氢量, 其中La1.5Ni0.5Mg17在573 K时吸放氢量分别为5.40和5.15 mass% H. 在553 K下, 体系α-β相区在600 s之内吸放氢反应分数均大于91%, 随着含Ni量的增加材料储氢容量降低, 吸放氢速率增大.物相分析知道体系吸氢后的主相是MgH2, 放氢后主相为Mg, 同时存在Mg2Ni, LaNi5或LaH3等催化物质, 从而使材料的氢化动力学性能得以明显改善.     

Layered hydride CaNiGeH with a ZrCuSiAs-type structure: crystal structure, chemical bonding, and magnetism induced by Mn doping

Stimulated by the discovery of the iron oxypnictide superconductor with ZrCuSiAs-type structure in 2008, extensive exploration of its isostructural and isoelectronic compounds has started. These compounds, including oxides, fluorides, and hydrides, can all be simply recognized as valence compounds for which the octet rule is valid. We report herein the first example of a ZrCuSiAs-type hydride, CaNiGeH, which violates the octet rule. This hydride was synthesized by hydrogenation of the CeFeSi-type compound CaNiGe under pressurized hydrogen. Powder diffraction and theoretical simulation confirm that H enters into the interstitial position of the Ca(4) tetrahedron, leading to notable anisotropic expansion of the unit cell along the c axis. Density functional theory calculations indicate the modification of the chemical bonding and formation of ionic Ca-H bond as a result of hydrogen insertion. Furthermore, CaNiGeH shows Pauli paramagnetism and metallic conduction similar to that of CaNiGe, but its carrier type changes to hole and the carrier density is drastically reduced as compared to CaNiGe. Mn-doping at the Ni site introduces magnetism to both the parent compound and the hydride. The measurement demonstrates that hydrogenation of CaNi(1-x)Mn(x)Ge reduces ferromagnetic ordering of Mn ions and induces huge magnetic hysteresis, whereas the spin glass state observed for the parent compound is preserved in the hydride. The hydrogenation-induced changes in the electric and magnetic properties are interpreted in terms of development of two-dimensionality in crystal structure as well as electronic state.     

RhCo双金属催化剂的研究III. Rh+Co/Al2O3上表面羰基氢化物及其动态行为

利用连续流动微反研究了Rh+Co/Al2O3催化剂的CO加氢反应, 结果表明反应在220℃以上发生, 反应活性随着温度的升高和H2/CO值的增加而增加。利用TP-IR动态方法研究了Rh+Co/Al2O3上CO和H2共吸附及其动态行为。结果表明在Rh+Co/Al2O3的孪生及线式中心上, CO和H2室温共吸附时即有部分孪生及线式CO转化为相应的羰基氢化物, 随着温度的升高, 剩余的孪生和线式CO继续向相应的羰基氢化物转化。而羰基氢化物则向多羰基氢化物转化。在到达反应温度之前, 催化剂表面只存在羰基氢化物及相应的多氢羰基氢化物。在反应温度则导致产物CH4生成。与CO加氢反应和CO歧化的吸附态研究结果相关联, 作者认为Rh+Co/Al2O3上CO加氢生成CH4是经由羰基氢化物-多氢羰基氢化物途径。     

Body centered cubic magnesium niobium hydride with facile room temperature absorption and four weight percent reversible capacity

We have synthesized a new metastable metal hydride with promising hydrogen storage properties. Body centered cubic (bcc) magnesium niobium hydride (Mg(0.75)Nb(0.25))H(2) possesses 4.5 wt% hydrogen gravimetric density, with 4 wt% being reversible. Volumetric hydrogen absorption measurements yield an enthalpy of hydride formation of -53 kJ mol(-1) H(2), which indicates a significant thermodynamic destabilization relative to the baseline -77 kJ mol(-1) H(2) for rutile MgH(2). The hydrogenation cycling kinetics are remarkable. At room temperature and 1 bar hydrogen it takes 30 minutes to absorb a 1.5 μm thick film at sorption cycle 1, and 1 minute at cycle 5. Reversible desorption is achieved in about 60 minutes at 175 °C. Using ab initio calculations we have examined the thermodynamic stability of metallic alloys with hexagonal close packed (hcp) versus bcc crystal structure. Moreover we have analyzed the formation energies of the alloy hydrides that are bcc, rutile or fluorite.     

Exploration of the nature of active Ti species in metallic Ti-doped NaAlH4

Clarification of the nature of active Ti species has been a key challenge in developing Ti-doped NaAlH(4) as a potential hydrogen storage medium. Previously, it has been greatly hindered by the invisibility of Ti-containing species in conventional analysis techniques. In the present study, for the first time, the catalytically active Ti-containing species have been definitely identified by X-ray diffraction in the hydrides doped with metallic Ti. It was found that mechanical milling of a NaH/Al mixture or NaAlH(4) with metallic Ti powder resulted in the formation of nanocrystalline Ti hydrides. The variation of the preparation conditions during the doping process leads to a slight composition variation of the Ti hydrides. The catalytic enhancement arising upon doping the hydride with commercial TiH(2) was quite similar to that achieved in the hydrides doped with metallic Ti. Moreover, the cycling stability that was previously established in metallic Ti-doped hydrides was also observed in the hydrides doped with TiH(2). These results clearly demonstrate that the in situ formed Ti hydrides act as active species to catalyze the reversible dehydrogenation of NaAlH(4). The mechanism by which Ti hydrides catalyze the reversible de-/hydrogenation reactions of NaAlH(4) was discussed.     

Magnetic and structural properties of Y6−xErxFe23 alloys and their hydrides

The magnetic characteristics and structural features of the Y_6?xEr_xFe₂₃ alloys and their hydrides are reported. The parent alloys all formed in a face-centered cubic structure. A pronounced minimum in the lattice parameter was observed for Er₄Y₂Fe₂₃. A similar minimum was also observed in the 1 atm hydrogen capacity of the alloys. The hydrides of the Y-rich compounds were found to retain the cubic structure of the parent compounds, whereas the hydrides of Er₅YFe₂₃ and Er₆Fe₂₃ adopt tetragonally distorted structures. Both the intermetallics and their hydrides were observed to be ferrimagnetic, exchange-dominated systems. In all cases, absorption of hydrogen resulted in an increase in both the saturation magnetization and the Curie temperature.     

Formation and characterization of water-soluble hydrido-ruthenium(II) complexes of 1,3,5-triaza-7-phosphaadamantane and their catalytic activity in hydrogenation of CO2 and HCO3- in aqueous solution

The water-soluble tertiary phosphine complex of ruthenium(II), [RuCl2(PTA)4], (PTA = 1,3,5-triaza-7-phosphaadamantane) was used as catalyst precursor for hydrogenation of CO2 and bicarbonate in aqueous solution, in the absence of amine or other additives, under mild conditions. Reaction of [RuCl2(PTA)4] and H2 (60 bar) gives the hydrides [RuH2(PTA)4] (at pH = 12.0) and [RuH(PTA)4X] (X = Cl- or H2O) (at pH = 2.0). In presence of excess PTA, formation of the unparalleled cationic pentakis-phosphino species, [HRu(PTA)5]+, was unambiguously established by 1H and 31P NMR measurements. The same hydrides were observed when [Ru(H2O)6][tos]2 (tos = toluene-4-sulfonate) reacted with PTA under H2 pressure. The rate of CO2 hydrogenation strongly depends on the pH. The highest initial reaction rate (TOF = 807.3 h(-1)) was determined for a 10% HCO3-/90% CO2 mixture (pH = 5.86), whereas the reduction was very slow both at low and high pH (CO2 and Na2CO3 solutions, respectively). 1H and 31P NMR studies together with the kinetic measurements suggested that HCO3- was the real substrate and [RuH(PTA)4X] the catalytically active hydride species in this reaction. Hydrogenation of HCO3- showed an induction period which could be ascribed to the slow formation of the catalytically active hydride species.     

Two new cluster ions, Ga[GaH3]4(5-) with a neopentane structure in Rb8Ga5H15 and [GaH2]n(n-) with a polyethylene structure in Rb(n)(GaH2)n, represent a new class of compounds with direct Ga-Ga bonds mimicking common hydrocarbons

The first examples of a new class of gallium hydride clusters with direct Ga-Ga bonds and common hydrocarbon structures are reported. Neutron powder diffraction was used to find a Ga[GaH(3)](4)(5-) cluster ion with a neopentane structure in a novel cubic structure type of Rb(8)Ga(5)H(15). Another cluster ion with a polyethylene structure, [GaH(2)](n)(n-), was found in a second novel (RbGaH(2))(n) hydride. These hydrocarbon-like clusters in gallium hydride materials have significant implications for the discovery of hydrides for hydrogen storage as well as for interesting electronic properties.     

Morphology-Dependent Stability of Complex Metal Hydrides and Their Intermediates Using First-Principles Calculations

Complex light metal hydrides are promising candidates for efficient, compact solid-state hydrogen storage. (De)hydrogenation of these materials often proceeds via multiple reaction intermediates, the energetics of which determine reversibility and kinetics. At the solid-state reaction front, molecular-level chemistry eventually drives the formation of bulk product phases. Therefore, a better understanding of realistic (de)hydrogenation behavior requires considering possible reaction products along all stages of morphological evolution, from molecular to bulk crystalline. Here, we use first-principles calculations to explore the interplay between intermediate morphology and reaction pathways. Employing representative complex metal hydride systems, we investigate the relative energetics of three distinct morphological stages that can be expressed by intermediates during solid-state reactions: i) dispersed molecules; ii) clustered molecular chains; and iii) condensed-phase crystals. Our results verify that the effective reaction energy landscape strongly depends on the morphological features and associated chemical environment, offering a possible explanation for observed discrepancies between X-ray diffraction and nuclear magnetic resonance measurements. Our theoretical understanding also provides physical and chemical insight into phase nucleation kinetics upon (de)hydrogenation of complex metal hydrides.     

Solvent-enhanced magnetic ordering temperature for mixed-valent chromium hexacyanovanadate(II), Cr(II)0.5Cr(III)[V(II)(CN)6].zMeCN, magnetic materials

The reaction of V(III)(THF)3Cl3 with NEt(4)CN in acetonitrile (MeCN) forms (NEt4)3[V(III)(CN)6].4MeCN (1), which after characterization was used as a molecular building block toward the synthesis of Prussian blue structured magnets. The reaction of 1 with [Cr(II)(NCMe)4](BF4)2 forms Cr(II)(0.5)Cr(III)[V(II)(CN)6].zMeCN via internal electron transfer, whose structure and magnetic properties are dependent on the degree of solvation, z. When solvated, Cr(II)(0.5)Cr(III)[V(II)(CN)6].1.2MeCN (2) is a mixture of crystalline and amorphous fractions that yield a material with two magnetic phases: bulk ferrimagnetic phase/crystalline [faced-centered-cubic lattice with a = 10.55(2) A] and cluster-glass phase/amorphous. The bulk ferrimagnetic phase exhibits a critical temperature, Tc, of 110 K, while the amorphous cluster-glass phase exhibits a freezing temperature, Tf, of approximately 25 K. Amorphous Cr(II)(0.5)Cr(III)[V(II)(CN)6].0.1MeCN (3) was determined to be the pure cluster-glass phase. This is an overall enhancement of 85 K (350%) in the magnetic ordering temperature via solvation, z. The coercivity was also increased 4-fold from 890 (2) and 3900 Oe (3) via desolvation.     

Catalytic Synthesis of Organolithium and Organomagnesium Compounds and of Lithium and Magnesium Hydrides—Applications in Organic Synthesis and Hydrogen Storage

A recent development in homogeneous catalysis is the discovery of catalysts that are active for the lithiation of 1-alkenes to alkenyllithium compounds and lithium hydride as well as for the hydrogenation of lithium and magnesium under mild conditions. The catalytically prepared magnesium hydride is highly reactive and adds to 1-alkenes to give diorganomagnesium compounds and can also be used in the preparation of, for example, silane and “active” magnesium. The use of metal hydrides in hydrogen storage is discussed: hydrogenation/dehydrogenation experiments show that the catalytically prepared magnesium hydride (which can be doped with a second metal) can be used as a high-temperature hydrogen storage material.