Ca2.9M0.1Co4O9 (M=Ag,La, Ba)复合氧化物体系的制备及电输运性能

采用柠檬酸溶胶-凝胶结合放电等离子烧结方法制备了p型Ca位掺杂的Ca2.9M0.1Co4O9(M=Ag, La, Ba)复合氧化物块体试样, 对其进行X 射线衍射(XRD)分析, 表明产物为单一物相, Ca位掺杂原子可以改变Ca2.9Co4O9多晶体的取向度, 掺杂试样取向度随着掺杂原子电负性的降低而提高|对其进行扫描电子显微镜(SEM)分析结果表明, 试样呈层状结构, 且层状结构随掺杂原子电负性降低而逐渐明显; 电性能分析结果表明, 测试温度范围内掺杂试样各温度点的电阻率随着掺杂原子电负性的降低而升高, 所有试样的载流子传输层未受影响, 导电机理未发生变化. 其中掺杂电负性最高的Ag原子的烧结体保持最低取向度的同时具有最低的电阻率, 在973 K时达6.87 mΩ·cm, 而掺杂电负性最低的Ba原子的烧结体具有高的取向度的同时具有较高的电阻率, 在973 K时达8.22 mΩ·cm.     

Al、Co和Mn掺杂对LiNiO2结构的影响

本文采用XRD和EXAFS研究Al、Co和Mn原子掺杂对LiNiO₂材料结构的影响。XRD结果表明掺杂材料具有与LiNiO₂相同的晶体结构，都属于R3m点群，但是晶胞略微缩小，LiNiO₂的层状结构得到改善,阳离子有序度增强。从EXAFS数据拟合结果可以看出，引入掺杂原子Al、Co和Mn减弱了Jahn-Teller畸变，使得NiO₆八面对称性提高。掺杂Al和Co使得第一壳层Ni-O配位键长减小，掺杂Mn原子影响不明显。Al、Co和Mn掺杂使第二壳层Ni-Ni配位键长减小，Co和Mn掺杂使得第二壳层局域有序度提高，而Al的引入使得第二壳层局域有序度降低。     

Eu2+/Mn2+激活的M3MgSi2O8-M2SiO4(M=Ba,Ca)荧光粉的发光特性

采用高温固相法制备了Eu2+/Mn2+单激活和共激活的M3MgSi2O8-M2SiO4(M=Ba,Ca)两相荧光粉.通过X射线衍射(XRD)和荧光光谱(PL)对样品材料的晶体结构和光谱性能进行了表征.XRD测试结果表明所合成的样品具有M3MgSi2O8和M2SiO4两种晶相结构.PL测试显示,Eu2+在Ba3MgSi2O8-Ba2SiO4体系中发射442和502nm两个波带的光;而Eu2+在Ca2+部分取代Ba2+的BaCa2MgSi2O8-Ba1.31Ca0.69SiO4体系中发射420～520nm的连续波带,并且激发光谱向长波扩展,更加适用于被InGaN芯片(395 nm)激发.通过改变Mn2+的掺杂量可制得颜色可调的BaCa2MgSi2O8-Ba1.31Ca0.69SiO4:Eu2+,Mn2+白光荧光粉.     

V2.1TiNi0．4Zr0．06Cu0．03M0．10（M=Cr，Co，Fe，Nb，Ta）储氢合金的微结构及电化学性能

采用磁悬浮感应熔炼方法制备了V2.1TiNi0.4Zr0.06Cu0.03M0.10(M=Cr,Co,Fe,Nb,Ta)(M=Cr,Co,Fe,Nb,Ta)储氢电极合金,通过X射线衍射(XRD)、扫描电了显微镜(SEM)、电子衍射能谱(EDS)分析和电化学测试等手段系统研究了添加元素M对合金微结构与电化学性能的影响.结果表明,所有合金均由BCC结构的V基同溶体主相和C14型Laves第二相组成,且第二相沿主相品界形成三维网状分布;Cr、Nb和Ta元素主要分布在合金主相中,而Co和Fe元素主要分布在第二相中.电化学性能测试表明,在V2.1TiNi0.4Zr0.06Cu0.03合金中掺加Cr、Co、Fe、Nb或Ta元素后,虽然会降低最大放电容量,但能有效抑制合金中V和Tj的腐蚀溶出,提高电极充放电循环稳定性;同时还能明显改善合金的高倍率放电性能.相比之下,V2.1TiNi0.4Zr0.06Cu0.03Cr0.10合金具有最佳的综合电化学性能.     

利用DFT方法探究一类自组装[Pt2M4（C≡CH）8]（M=Cu，Ag）簇合物的电子结构和光谱性质

应用TD．DFT（time－dependent density functional theory）并PCMfpolarizable continuum model）模型研究了一类自组装的[Pt2M4（C＇≡CH）8]（M=Cu,Ag）簇合物的电子结构和光谱性质．应用DFT（density functional theory）方法优化了该簇合物的基态及激发态结构．综合计算结果,得到与试验结果相一致的结构与光谱特点．[Pt2Ag4（C≡CH）8]具有呈D4和D4h对称性的两个稳定的基态几何结构．Pt－M距离预示弱相互作用的存在．Cu—Cu距离大于俩个Cu原子的范德华半径和而Ag－Ag间距与俩个Ag原子的范德华半径和差别不大．激发过程使得Pt…M,Ag…Ag作用增强,虽然Cu…Cu距离也相应缩短,但是其仍大于范德华半径之和．[Pt2Cu4（C≡CH）8]、[Pt2Ag4（C≡CH）8]（A）和（B）的最低能吸收在450、365和375nm处,发射在611、431和435nm处．红外可见谱范围内,[Pt2M4（C≡CH）8]的吸收波带都有Cu或Ag成分的贡献,所以没有ILCT或MPtLCT跃迁特征出现（ILCT：intraligand charge transfer;MLCT：metal-to—ligand charge transfer）．由于最低能吸收和发射具有不同的跃迁特征,所以发射不是来自于最低能吸收．[Pt2Ag4（C≡CH）8]簇合物的MM相互作用在激发态增强,发射光谱具有显著的ILCT特点,这也是[Pt2Ag4（C≡CH）8]的发射波长相对于其对应的同配体前躯体[Pt（C≡CH）4]^2-有少许蓝移的原因．     

Ca掺杂的Ba2Al2Si10N14O4:Eu2+荧光粉发光性能

通过固相反应制备了系列Ca掺杂的Ba2Al2Si10M14O4:Eu2+色荧光粉,发现当半径较大的Ba被Ca取代后导致了晶格的收缩,通过X射线衍射(XRD)测量和Unitcell软件计算发现Ca的最大掺杂量在20％.Ca掺人Eu0.4Ba1.6Al2Si10N14O4荧光粉后,可有效地提高光转换性能,并使激发光谱发生一定程度的红移和宽化,从而被近紫外宽波段光有效激发,与近紫外LED的发射光谱匹配.同时Ca的掺杂也使发射光谱发生了可控的红移,可以由520 nm的绿光红移至548 nm的黄光区域.进一步发现Eu2+的淬灭浓度随着20％ Ca的掺入而降低,这是由于Ca掺入导致的晶格收缩使Eu2+离子间距离减小.最后在CIE色度图中对不同Ca,Eu浓度的荧光粉的色坐标位置进行比较,发现可通过Ca,Eu浓度的变化在很大范围内调制荧光粉的发光性能.     

V2O5/MO-Al2O3（M = Mg，Ca，Sr，Ba）催化剂用于正丁烷催化氧化脱氢反应

采用浸渍法制备了不同V2O5担载量的V2O5/MO-Al2O3(M = Mg, Ca, Sr, Ba)催化剂,钒物种的前驱体为偏钒酸铵.对制备的催化剂进行了一系列表征,并对催化剂上正丁烷选择性氧化脱氢制取丁烯进行了反应研究.表征结果(包括比表面积、X射线衍射、傅里叶红外光谱、氢气程序升温还原和拉曼光谱)显示,不同碱土金属元素掺杂的催化剂显示不同的钒价态信息和催化性能.其中掺杂Ca, Sr, Ba的催化剂,正钒酸盐相很难被还原,因此催化剂的氧化还原循环难以建立,导致以上三种催化剂在正丁烷氧化脱氢反应中活性较低.然而, Mg掺杂的催化剂却显示出较高的催化活性和选择性.实验结果表明：在Mg掺杂的载体上担载5% V2O5的催化剂上600°C时可获得高达30.3%的正丁烷转化率和64.3%的烯烃总选择性.这与V2O5担载量为5%时,在获得高度分散的钒氧化合物物种时可使MgO晶相稳定存在密切相关.     

硅基稀土掺杂团簇MSi_7~q(M=Eu,Sm,Yb;q=0,-1)结构预测与光电子能谱研究

采用随机踢球模型结合密度泛函理论,在PBEPBE/RE/SDD/Si/6-311+G(d)水平下研究了中性和阴性的硅基稀土掺杂团簇MSi_7~q(M=Eu,Sm,Yb;q=0,-1)的几何结构、稳定性及电子和磁学性质.计算结果表明,阴性团簇的基态结构是在五角双锥的双锥侧面外法向方向加入一个Si原子而形成的3D结构,并且稀土原子M处于五角双锥的顶点;中性团簇的最低能结构是一个畸变的双帽八面体,并且M原子处于八面体的赤道面上.SmSi_7~-团簇在这3种稀土掺杂的团簇中具有最高的平均结合能和掺杂能,是这3种稀土掺杂团簇中最稳定的一种.Si_7团簇是非磁性团簇,但是当M原子(M=Eu,Sm,Yb)掺入其中时,由于镧系元素独特的原子磁性,使其变成了磁性团簇.此外,还模拟了各团簇前几种低能异构体的光电子能谱.     

层状钴氧化物Bi2-xAgxSr2Co2O8-δ的高温热电性能及XPS研究

采用固相反应法制备了组成为Bi2-xAgxSr2Co2O8-δ（x=0.0,0.4,0.8,略写为BAC-222）的层状钴氧化物陶瓷。利用X-射线光电子能谱考察该类化合物的电子结构,结果表明钴离子以Co^3＋和Co^4＋混合价态形式存在,nCo^4＋/nCo^3＋的比例随着Ag掺杂的量增加而增加。O1s光电子谱显示在所有样品中均存在点阵氧和吸附氧。热电性能测试结果显示,随着Ag掺杂量的增加,电导率显著增加而Seebeck系数几乎保持不变,Ag的引入极大的影响了BAC-222的电子输运性质,其功率因子在1123K时达到了1.23×10^-4W·m^-1·K^-2,是一种具有很好应用前景的热电材料。     

人中白矿物元素含量分析

用原子吸收分光光度法测定了中药人中白中 1 2种矿物元素含量。结果表明 ,人中白中Ca、Mg、Ba、K和Na的含量在 1× 1 0 3以上 ,而Fe、Cr、Mn的含量在 1 0× 1 0 6 ～ 1 0 0 0× 1 0 6 范围内 ;Ni、Se浓度也超过 1 0× 1 0 6 ,Cu、Co的含量也在 5× 1 0 6 以上。     

Zintl-Verbindungen mit Gold: M3AuSn4 mit M = K,Rb, Cs und M3AuPb4 mit M = Rb,Cs

Zintl-Compounds with Gold: M₃AuSn₄ with M = K, Rb, Cs and M₃AuPb₄ with M = Rb, Cs Silver coloured, brittle single crystals of the compounds M₃AuSn₄ with M = K, Rb, Cs and M₃AuPb₄ with M = Rb, Cs were synthesized by reactions of alkali metal azides (MN₃) with gold sponge and tin (lead) powder at T = 923 K. The structures of the isotypic compounds (space group Pmmn, Z = 2) were determined from X-ray single-crystal diffractometry data (see ‘‘Inhaltsübersicht”︁”︁). The Zintl-compounds M₃AuE(14)₄ with E(14) = Sn, Pb contain [AuE(14)₄]-chains with P₄-analogous E(14)₄-tetrahedra which are connected by μ₂-bridging gold atoms.     

Relativistic-consistent electron densities of the coinage metal clusters M2, M4, M4(2-), and M4Na2 (M = Cu, Ag, Au): a QTAIM study

We employ second-order M?ller-Plesset perturbation theory level in combination with recently developed pseudopotential-based correlation consistent basis sets to obtain accurate relativistic-consistent electron densities for small coinage metal clusters. Using calculated electron densities, we employ Bader's quantum theory of atoms in molecules (QTAIM) to gain insights into the nature of metal-metal bonding in the clusters M(2), M(4), M(4)(2-), and M(4)Na(2) (M = Cu, Ag, Au). For the simplest case of the metal dimer, M(2), we correlate the strength of the metal-metal bond with the value of the electron density at the bond critical point, the total energy density at the bond critical point, the sharing (delocalization) index, and the values of the two principle negative curvatures. We then consider changes to the metal-metal bonding and charge density distribution upon the addition of two metal atoms to form the metal tetramer, M(4), and then followed by the addition of an electron pair to form M(4)(2-) and finally followed by the addition of two alkali metal (sodium) ions to form M(4)Na(2). Using topological properties of the electron density, we present evidence for the existence of σ-aromaticity in Au(4)(2-). We also report the existence of two non-nuclear attractors in the molecular graph of Cu(4)(2-) and large negative charge accumulation in the nonbonded Cu basins of this cluster.     

Ti-48Al-2M~1-2M~2(M~1=Nb,V;M~2=Mn,Cr,V)合金电子结构

用紧束缚能带计算方法(EHT)研究了标题多元合金的能带及电子结构。发现少量的多种元素在γ-TiAl中掺杂,对合金中电荷分布的影响,具有单种元素掺杂的叠加性;选择适当的合金元素就能达到多种掺杂的性能互补。多种元素掺杂能更有效地使成键电子云趋势于球形化,Peierls力均称为化,有利于增加γ-TiAl合金的塑性和变形性。     

Heterodinuclear M1M2 Complexes (M1=Ni,Pd, Pt; M2=Rh,Ir) Supported by a Tetradentate Phosphine Ligand and Their Application for Hydrosilylation

A new series of cationic heterodinuclear complexes, [M¹M²Cl₂(meso-dpmppp)(RNC)₂]PF₆ (M¹=Ni, M²=Rh, R=^tBu ( 1 a ); M¹=Pd, M²=Rh, R=^tBu ( 2 a ), Xyl ( 2 b ); M¹=Pt, M²=Rh, R=^tBu ( 3 a ), Xyl ( 3 b ); M¹=Pd, M²=Ir, R=^tBu ( 4 a )), supported by a tetradentate phosphine ligand, meso-Ph₂PCH₂P(Ph)(CH₂)₃P(Ph)CH₂PPh₂ (meso-dpmppp), were synthesized by stepwise reactions of meso-dpmppp with NiCl₂ ⋅ 6H₂O or MCl₂(cod) (M=Pd, Pt), forming mononuclear metalloligands of [M¹Cl₂(meso-dpmppp)], and with [M²Cl(cod)]₂ (M²=Rh, Ir) and RNC (R=^tBu, Xyl) in the presence of [NH₄][PF₆]. The related neutral PdRh complex, [PdRhCl₃(meso-dpmppp)(XylNC)] ( 5 ), was also prepared. The structures of 1 – 5 were determined by X-ray analyses to contain two square planar d⁸ metal centers with face-to-face arrangement, where meso-dpmppp supports M¹ and M² metal ions in cis/trans-P,P coordination mode, combining cis-{M¹P₂Cl₂} and trans-{M²P₂(CNR)₂} units. Complexes 1 – 4 showed an intence characteristic absorption around 422–464 nm derived from Rh^I→RNC MLCT transition (HOMO→LUMO+1), which are influenced by changing M¹ (Ni^II, Pd^II, Pt^II) metal ions since HOMO composed of dσ* orbitals appreciably destabilized by changing M¹ from Ni to Pd, and Pt. The electronic structures of 1 a – 4 a were investigated on the basis of DFT calculations and NBO analyses to show weak but noticeable d⁸–d⁸ metallophilic interaction as empirical dispersion energy of 0.9–1.5 kcal/mol without M¹–M² covalent bonding interaction. In addition, 1 – 5 were utilized as catalysts for hydrosilylation of styrene, and the NiRh complex 1 a was found to show higher activity and chemo- and regioselectivity compared with 2 – 5 .     

Heterocyclic compounds M1M2E1E2H8 (M1, M2 = Al,Ga, In; E1, E2 = N,P, As): A quantum chemical study

Structural and thermodynamic characteristics of heteroelement inorganic heterocycles M¹M²E¹E²H₈ (M¹, M² = Al, Ga, In; E¹, E² = N, P, As) were calculated by the density functional theory B3LYP/LANL2DZ(d,p) method. It was shown that energetic characteristics of heterocycle dissociation processes can be calculated by simple a additive scheme with the use of the average M-E bond energy. Dissociation of heteroelement heterocycles into monomeric H₂MEH₂ molecules proceeds according to the hardsoft acid-base (HSAB) concept.     

Electronic Structure of TiAl-2M(M=V,Nb,Ta,Cr,Mo,W,Mn) Alloy

1INTRODUCTIONTitaniumaluminidesbasedonY-TiAlarereceivingconsiderableattentionaspo-tentialcandidatesformaterialsinhightemperatureaerospaceapplication.Theirlowdensity,hightemperaturescreepresistance,highoxidationresistanceandstrengthmakesthemexcellentpotentialenginematerials.Howevertheirlowductilityandlowfracturetoughnessatroom'temperaturesaremajorhindrancestotheirpracticaluti-lization.TheTiAlalloymayhaveanelongationabout2%t'},furtherimprovementisnecessarybeforethesematerialscouldbeusedin…     

Ab initio pseudopotential study of M2As− and M2Br+ (M = Cu,Ag, Au)

The equilibrium geometries and the vibration frequencies of M₂As⁻ and M₂Br⁺ (M = Cu, Ag, Au) are calculated at the Hartree–Fock (HF) and the second‐order Møller–Plesset (MP2) levels with pseudopotentials. The calculated results indicate that the species have a bent structure (C_2v). The electron correlation corrections on the geometrical structure are investigated at the MP2 level, the bond angles are reduced by 10°–20° for considered species. The electron correlation effects on the geometry of the Au₂As⁻ are studied particularly at MP2, MP3, MP4, CCSD and CCSD(T) levels. Comparing the species containing Ag and Au, the relativistic effects slightly short the bond lengths of the species. The bonding possibility of the Au₂As⁻ is predicted. © 2000 John Wiley & Sons, Inc. Int J Quant Chem 80: 38–43, 2000