RFe_(11)Ti和RFe_(10)Si_2(R=Y、Gd、Dy)合金的磁性研究

研究了°RFe_(11)Ti(R=Y,Gd,Dy)和RFe_(10)Si_2(R=Gd,Dy)合金的~(57)Fe室温穆斯堡尔诺。研究表明,结构稳定化元素硅原子能使合金的饱和磁化强度有所提高,也可增加合金的居里温度。GdFe_(11)Ti合金具有较其它合金大的超精细场。富铁稀土合金的~(57)Fe穆斯堡尔谱超精细场应考虑稀土原子的5d6s电子对铁原子的影响。     

ZrO2-10% Dy2O3纳米晶的碱性水热法合成及其烧结体的电性能研究

以湿化学法制得Zr(OH)4和Dy(OH)3的共沉淀为前驱体, 在碱性介质(pH=7.60～13.89)中用水热法合成了ZrO2-10% Dy2O3(摩尔分数)立方相纳米晶. 研究发现, 纳米晶粒径随着反应介质pH值的增大而增大;同时纳米晶粒径随着水热反应介质温度的升高而增大. 将ZrO2-10% Dy2O3纳米晶在1400 ℃下烧结制得了致密的固体电解质陶瓷样品, 比通常高温固相反应法采用的烧结温度(＞1550 ℃)降低了150 ℃以上. 还用交流阻抗谱法及氧浓差电池法研究了ZrO2-10% Dy2O3陶瓷样品在600～1000 ℃下的离子导电特性. 结果表明, 该陶瓷样品在600～1000 ℃下氧离子迁移数为1, 氧离子电导率的最大值为2.2×10-2 S·cm-1, 是一个优良的氧离子导体.     

新的溶胶-凝胶法制备Ge/SiO2量子点玻璃

以3－三氯锗丙酸和正硅酸乙酯为原料,通过水解、缩聚凝胶热处理及氢气反应,在SiO2凝胶玻璃中析出立方相Ge纳米晶,当x=30时,凝胶玻璃中除了析出立方相Ge纳米晶处,还析出六方相GeO2,利用XRD测试了Ge纳米晶的大小,发现随着掺杂量的增加,纳米颗粒粒径从1nm增大到10nm,电子衍射表明镶嵌在SiO2凝交玻璃中的Ge纳米晶为多晶结构。     

X型六角晶系钡铁氧体纳米晶的制备和表征

用硬脂酸凝胶法制备了Co₂-X型六角晶系钡铁氧体纳米晶,在750℃热处理得到的纳米晶形貌为球形,粒径范围为15～25nm.随着热处理温度的升高,粒子逐渐长大并呈块状.振荡样品磁强计测试结果表明,Co₂-X型六角晶系钡铁氧体纳米晶具有与常规体材料不同的磁性能,其比饱和磁化强度σ_s低于后者.产物的矫顽力、比饱和磁化强度随粒子的长大呈规律性的变化.     

Nd_(1-y)Dy_yFe_(11-x)TiM_x(M=Mo,Si)系列化合物中Mo,Si元素的掺杂对其结构及磁性能的影响

通过电弧方法制备了一系列的Nd1-yDyyFe11-xTiMx(M=Mo,Si)型稀土过渡金属化合物,并且通过X射线衍射和中子衍射对其晶体结构进行了研究.实验发现,Nd1-yDyyFe11-xTiMx(M=Mo,Si)系列中化合物主要结构为ThMn12-type(1︰12相).Dy取代Nd没有明显影响1︰12相形成的含量.在Nd0.5Dy0.5Fe11-xTiMx(M=Mo,Si)系列中,当x≤0.8时Nd0.5Dy0.5Fe11-xTiMox化合物主要呈ThMn12-type晶形,当x0.8时,化合物中1︰12相的含量降至80%以下;对于Nd0.5Dy0.5Fe11-xTiSix,当x≤0.6时,Nd0.5Dy0.5Fe11-xTiSix化合物主要呈ThMn12-type晶形,当x0.6时,化合物中1︰12相的含量降至90%以下但保持在80%以上.在不同的化合物中,稳定元素的含量不同.ThMn12-type相的百分含量随着Mo和Si取代Fe含量的增加而减小,意味着Mo和Si取代更多的Fe时,ThMn12-type相将变得不稳定.Nd0.5Dy0.5Fe11-xTiMox化合物的晶格参数a和c以及晶胞体积V随着Mo(x)含量的增加呈线性增加是因为Mo的原子半径比其中的Fe的大;而Nd0.5Dy0.5Fe11-xTiSix合金的晶格参数a和c以及晶胞体积V随着Si(x)含量的增加呈线性减小是因为Si的原子半径比其中的Fe的小.在NdyDy1-yFe11-xTiMx(M=Mo,Si)中,因为Ti和Mo的半径比Fe大而Si的半径比Fe小,所以Ti和Mo原子优先占据8i晶位,Si原子优先占据8j和8f晶位.在化合物RFe12-xMx中,居里温度由T-T交换作用决定的,由于T-T交换作用依赖于T-T原子距离,因此其他元素对Fe的取代导致了居里温度的改变.磁性测量表明Mo或Si取代Fe均导致居里温度的降低.     

SrAl_2O_4∶Eu~(2 ),Dy~(3 )纳米长余辉发光材料的制备与表征

采用溶胶鄄凝胶法制备了SrAl2O4∶Eu2 ,Dy3 纳米长余辉发光材料,研究了pH值、反应温度和络合剂等对溶胶鄄凝胶形成的影响,研究了灼烧温度对SrAl2O4∶Eu2 ,Dy3 晶相、颗粒尺度和发光性能的影响。利用XRD,SEM,光谱分析等手段对产物进行了结构和性能分析。实验结果表明,在800℃时SrAl2O4晶相开始形成但没有发光,而在1100℃烧结的样品则具有很好的发光性能。样品平均晶粒尺寸随灼烧温度升高而增加,平均晶粒尺寸为20~40nm。样品的激发光谱是峰值在240,330,378和425nm的连续宽带谱,发光光谱是峰值在523nm的宽带谱,与SrAl2O4∶Eu2 ,Dy3 粗晶材料相比,发光光谱发生了“红移”现象。样品的热释光峰值位于157℃,与SrAl2O4∶Eu2 ,Dy3 粗晶材料相比,峰值向低温移动了13℃。     

RFe12—xMx金属间化合物的磁性研究

用磁测量和X射线衍射方法研究了1:12型RFeM(M=V或Ti)的结构和内禀磁性。X射线衍射实验表明,它们属ThMn_12型体心四方结构。晶格常数的变化与形成结构的各元素的大小变化规律一致。居里温度主要由3d-3d、3d-4f原子的交换作用决定,用平均场拟合的数据与实验值符合较好。从饱和磁化强度的变化来看,铁与轻稀土磁矩为铁磁耦合,与重稀土磁矩为反铁磁耦合。在低温各向异性场由稀土子晶格决定。文章中还研究了钴、镍替代部分铁后对磁性能的影响。     

巡游磁体Sr1-xCaxRuO3系列的磁性

固相反应法制备了Sr1-xCaxRuO3系列. PPMS测量了样品的零场冷却和加场冷却磁化强度和交流磁化率. 居里-外斯定律确定了样品的顺磁居里温度TP. 结果表明, 随x的增加, TP减小. 当x≤0.6时TP大于零; 当x>0.6时TP小于零. 利用交流磁化率随温度变化的关系确定样品的铁磁居里温度TC, 随x的增加TC减小. 当x=0.8时TC降至4 K; 而当x=1.0时, 即使温度降到1.7 K, 也未出现磁有序.     

钙钛矿锰氧化物(La_(1-x)Gd_x)_(0.5)Sr_(0.5)MnO_3的磁电阻效应

采用传统的高温固相法制备了多晶样品(La1-xGdx)0.5Sr0.5MnO3(x=0,0.1,0.2,0.3,0.4),利用X射线衍射仪(XRD)、超导量子磁强计(SQUID)、标准四端引线法分别对样品结构、磁性、电性以及磁电阻效应进行了研究。研究表明:Gd的少量替代并没有引起结构变化;随着Gd含量的增加,所有样品的居里温度TC和金属-绝缘体转变温度Tp都降低了;在TC附近发现了磁电阻效应,同时在低温下发现了更大的磁电阻;并且Gd的少量替代可使磁电阻MR增大。     

原子级壳层厚度Ru@Pt核壳结构纳米粒子的制备与表征

采用连续多元醇法,以RuCl₃·xH₂O和PtCl₂为前驱体,乙二醇为还原剂,聚乙烯吡咯烷酮为稳定剂的反应体系,并通过调节PtCl₂用量和还原温度成功制备了壳层厚度约为1.5个Pt原子层的单分散Ru@Pt核壳结构纳米粒子,利用透射电子显微镜(TEM)、X射线衍射仪(XRD)、X射线光电子能谱仪(XPS)等分析方法对其微观结构、粒径分布、晶型结构、物相组成进行了表征。 结果表明,该纳米粒子分布均匀且基本为球形,平均粒径约为3.57 nm,其中内核直径约为2.49 nm,外壳厚度约为0.55 nm,壳层金属Pt具有很好的晶型,Pt原子主要为{111}晶面,内核金属Ru与外壳金属Pt互相产生了电子效应使Pt的衍射峰和Ru、Pt的电子结合能产生了一定偏移,并初步研究了有效控制该核壳结构纳米粒子壳层厚度和增强核与壳两种金属之间电子效应的因素,使其有望在催化等领域发挥潜在的应用价值。     

单掺杂与共掺杂离子对Sr2Mg(BO3)2磷光体热释发光的影响

通过高温固相法合成了Sr2Mg(BO3)2磷光体, 并研究了Li＋, Bi3＋, Gd3＋, Ti4＋共掺杂对Sr2Mg(BO3)2∶Dy磷光体热释发光的影响. 研究发现: Li＋的共掺杂使Sr2Mg(BO3)2∶Dy磷光体的热释光主峰强度增加, 而 Bi3＋, Gd3＋或Ti4＋的掺入使样品的热释光强度降低. 在Li＋, Bi3＋, Gd3＋或Ti4＋共掺杂的Sr2Mg(BO3)2∶Dy磷光体高温热释光发射谱中, 我们观察到了480, 579, 662和755 nm的发射峰, 为特征Dy3＋离子的4F9/2→6H15/2, 4F9/2→6H13/2, 4F9/2→6H11/2和4F9/2→6H9/2跃迁, 与Sr2Mg(BO3)2∶Dy磷光体的发射一致. 利用峰形法, 我们评估了Sr2Mg(BO3)2∶ , ( )热释光磷光体234 ℃发光峰的动力学参数, 陷阱深度E＝1.1 eV, 频率因子s＝6.3×109 s－1, 遵循二级动力学.     

Gd7Pd3-xFex合金磁性及磁热效应的研究

采用电弧熔炼和高温退火的方法制备了Gd7Pd3-xFex(x=0, 0.2, 0.5, 0.8和1)合金材料,并对该系列合金材料的磁特性及磁热效应进行了研究。X射线粉末衍射研究表明,所有的材料均形成Th7Fe3型结构。并且随着x的增大,晶格常数、居里温度、饱和磁化强度和最大磁熵变均有所降低。相比于Gd7Pd3,掺入Fe元素的材料可以获得更接近室温的居里温度和更宽的工作温区,从而导致了7 T磁场下高达1096 J·kg^-1的相对制冷能力(RCP), Gd7Pd3-xFex有望被用于室温附近的磁制冷。     

Use of dispersive liquid-liquid microextraction for simultaneous preconcentration of samarium,europium, gadolinium and dysprosium

A new preconcetration method of dispersive liquid-liquid microextraction (DLLME) was developed for simultaneous preconcentration of samarium, europium, gadolinium and dysprosium. DLLME technique was successfully used as a sample preparation method. In this preconcentration method, an appropriate mixture of extraction solvent, disperser solvent was injected rapidly into an aqueous solution containing Sm, Eu, Gd and Dy after complex formation using chelating reagent of the 1-(2-pyridylazo)-2-naphthol (PAN). After phase separation, 0.5 mL of the settled phase containing enriched analytes was determined by inductively coupled plasma optical emission spectrometry (ICP-OES). The main factors affected the preconcentration of Sm, Eu, Gd and Dy were extraction and dispersive solvent type and their volume, extraction time, volume of chelating agent (PAN), centrifuge speed and drying temperature of the samples. Under the best operating condition simultaneous preconcentration factors of 80, 100, 103 and 78 were obtained for Sm, Eu, Gd and Dy, respectively.     

(Gd1-xREx)5Si4(RE=Dy, Ho)系列材料磁熵变研究

对 (Gd1-xDyx)5Si4(x=0.1, 0.2, 0.3, 0.35) 和(Gd1-xHox)5Si4(x=0.05, 0.15, 0.25)系列合金的居里温度、磁相变、磁熵变等磁性质进行了研究. 结果发现 该系列合金保持了Gd5Si4的Sm5Ge4正交型晶体结构, 居里温度随着引入的x量的增加而呈近似线性减小趋势;在居里温度附近样品的磁特性符合二级相变规律;通过调节Dy 或Ho的含量调节居里点, 样品中不含贵重元素Ge, 大大降低了成本;在较宽的温度范围和低场下(＜2 T)具有较大的磁熵变值从而使其适合于被制成梯度功能复合材料. 研究表明 (Gd1-xREx)5Si4(RE=Dy, Ho)系列材料有望成为较好的室温低场磁制工质.     

A Luminescent and Sublimable Dy(III) -Based Single-Molecule Magnet

The reaction of [Ln(hfac)(3) ]?2?H(2) O and pyridine-N-oxide (PyNO) leads to isostructural dimers of the formula [Ln(hfac)(3) (PyNO)](2) (Ln=Eu, Gd, Tb, Dy). The Dy derivative shows a remarkable single-molecule magnet behavior with complex hysteresis at 1.4?K. The dynamics of the magnetization features are two relaxation regimes: a thermally activated one at high temperature (τ(0) =(5.62±0.4)×10(-11) s and Δ=(167±1)?K) and a quantum tunneling regime at low temperature with a tunneling frequency of 0.42?Hz. The analysis of the Gd derivative evidences intradimer antiferromagnetic interactions (J=(-0.034±0.001)?cm(-1) ). Moreover, the Eu, Tb, and Dy derivatives are luminescent with quantum yield of 51, 53, and 0.1?%, respectively. The thermal investigation of [Dy(hfac)(3) (PyNO)](2) shows that the dimers can be sublimated intact, suggesting their possible exploit as active materials for surface-confined nanostructures to be investigated by fluorimetry methods.     

Luminescence of RE~(3+) and energy transfer from Gd~(3+) to RE~(3+) (RE = Dy, Eu) in SrGdAlO_4:RE~(3+)

Spectral properties of Gd3+, Dy3+ and Eu3+ ions in SrGdAlO4 are reported in detail. A cooperative vibronic transition of Gd3+ and the emission from the higher 5DJ (J=1, 2, 3) levels of Eu3+ were observed. Energy transfer occurs from Gd3+ to Dy3+ and to Eu3+. The influence of Gd3+ and Dy3+ concentrations on the luminescence intensity is discussed.     

Synthesis and magnetism of rare earth (Nd,Gd,Dy,Ho,Er,Y) pentafluoropropionate binuclear complexes with 2-(4''''-methoxy-phenyl)-4,4,5,5-tetramethylimidazoline-1-oxyl-3-oxide

Six compounds of the general formula [Ln(pfpr)3]2(NITPhOMe).nH2O, where Ln=Nd, Gd, Dy, Ho, Er, Y, pfpr=pentafluoropropionate, NITPhOMe=2-(4'-methoxyphenyl)-4,4,5, 5-tetra-methylimidazoline-1-oxyl-3-oxide, and n=4 (for Nd, Dy, Er); 3 (for Gd); 6 (for Ho); 5 (for Y), have been synthesized. These complexes were characterized by elemental analyses, IR, electronic spectra and molar conductances. The variable temperature (4-300 K) magnetic susceptibility of the complex [Gd(pfpr)3]2(NITPhOMe).3H2O was determined. The observed susceptibility data were fit to those from theoretical magnetic equation by least-squares method. The exchange integral, J, was found to be equal to 2.14 cm-1. This indicates a weak ferromagnetic spin-exchange interaction between the radical and the gadolinium(III) ion.     

A new family of octanuclear Cu4Ln4 (Ln = Gd, Tb and Dy) spin clusters

The reaction of Cu(OAc)2 and Ln(OAc)3 (Ln = Gd, Tb and Dy) with 2-amino-2-methyl-1,3-propanediol (ampdH2) under solvothermal conditions has afforded a new family of isostructural octanuclear Cu4Ln4 complexes with the formula [Cu4Ln4(OAc)12(ampdH)8(OH2)2] (Ln = Gd (1), Tb (2) and Dy(3)) in good yield. Variable temperature magnetic susceptibility measurements reveal weak intramolecular exchange interactions for 1 and 2. Ferromagnetic coupling is observed for 1 and attributed to Cu...Gd interactions. In contrast, the magnetic susceptibility behaviour of 2 arises from a combination of intramolecular exchange interactions and the crystal field splitting of the (7)F6 ground state of the Tb(III) ions.     

Synthesis,Structure and Mechanism of a Series of Novel Nanocrystalline Rare Earth Orthovanadate Catalysts for Oxidative Dehydrogenation of Light Alkanes at Low Temperatures

The oxidative dehydrogenation of light alkanes to light alkenes is one of the potentially important catalytic processes for the effective utilization of light alkanes. However, high temperatures were required to initiate the reactions on heterogeneous catalysts reported by other authors in the literature^[1,2]. In recent years we reported a series of novel nanocrystalline rare earth orthovanadates synthesized by the peroxyl and nitrate methods for oxidative dehydrogenation of propane at low temperatures^[3,4]. In this paper the synthesis of a series of novel nanocrystalline rare earth orthovanadates (LnVO₄, Ln=Y, La, Ce, Pr, Nd, Sm Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb) by the citrate method is reported, together with the structural characterization and excellent performances of the catalysts for oxidative dehydrogenation of light alkanes.     

Synthesis, characterization, and thermal properties of homoleptic rare-earth guanidinates: promising precursors for MOCVD and ALD of rare-earth oxide thin films

Eight novel homoleptic tris-guanidinato complexes M[(N(i)Pr)(2)CNR(2)](3) [M = Y (a), Gd (b), Dy (c) and R = Me (1), Et (2), (i)Pr (3)] have been synthesized and characterized by NMR, CHN-analysis, mass spectrometry and infrared spectroscopy. Single crystal structure analysis revealed that all the compounds are monomers with the rare-earth metal center coordinated to six nitrogen atoms of the three chelating guanidinato ligands in a distorted trigonal prism geometry. With the use of TGA/DTA and isothermal TGA analysis, the thermal characteristics of all the complexes were studied in detail to evaluate their suitability as precursors for thin film deposition by MOCVD and ALD. The (i)Pr-Me(2)N-guanidinates of Y, Gd and Dy (1a-c) showed excellent thermal characteristics in terms of thermal stability and volatility. Additionally, the thermal stability of the (i)Pr-Me(2)N-guanidinates of Y and Dy (1a, c) in solution was investigated by carrying out NMR decomposition experiments and both the compounds were found to be remarkably stable. All these studies indicate that (i)Pr-Me(2)N-guanidinates of Y, Gd and Dy (1a-c) have the prerequisites for MOCVD and ALD applications which were confirmed by the successful deposition of Gd(2)O(3) and Dy(2)O(3) thin films on Si(100) substrates. The MOCVD grown films of Gd(2)O(3) and Dy(2)O(3) were highly oriented in the cubic phase, while the ALD grown films were amorphous.