掺杂铬对NiFe2O4的磁性和结构稳定性影响

利用物理特性测试仪对共沉淀法制备的Cr3+掺杂NiFe2O4的磁性能进行测试,发现掺杂Cr3+并经350、 600℃焙烧的NiFe2O4样品,饱和磁化强度Ms和剩磁Mr随掺杂量的增加而下降,矫顽磁场强度Hc随掺杂量的增加而增加.XRD平均晶粒测试结果显示,样品的平均晶粒大小随掺杂量的增加而减小.在共沉淀过程掺杂的Cr3+经600℃热处理后已进入NiFe2O4晶格.晶格中的Cr3+对NiFe2O4分解CO2的H2/CO2循环反应性能产生很大影响,纯NiFe2O4循环反应15次失活,而掺4%Cr3+的NiFe2O4循环反应50次仍然具有活性.     

铝锂混合掺杂尖晶石相Li_(1+x)Al_yMn_(2-y)O_4材料结构性能的研究

采用一种简单的合成工艺 ,将铝和锂混合掺入到主尖晶石相锰酸锂中 ,研究不同掺杂铝量对材料的初始容量及循环稳定性能的影响 .结果表明同时掺杂铝锂的材料要比单独掺杂铝或锂的循环稳定性好 .利用扫描电镜、粉末X_射线衍射仪、红外光谱仪对材料形貌及结构进行研究 ,结果表明所合成的掺杂铝锂材料颗粒细小、分布均匀 ,具有较好的结晶性能 ,较高的初始容量和良好的循环稳定性 ,其初始容量达 119mAh/g ,循环 2 0 0次后容量仍然保持在 10 6mAh/g     

Structural Dependence of Magnetic and Transport Properties in Doped Manganite Perovskites

1 INTRODUCTION In recent years, ABO3-type perovskite-like manganites, RE1xDxMnO3 (RE = rare earth ions, D = Ca2+, Sr2+, Ba2+ etc.), have inspired remarkable attention due to the colossal magnetoresistance (CMR) effects for fundamental and practical consideration [1, 2]. Since A- and B-site substitution can give rise to a large number of derivant compounds, fruitful structural, magnetic and transport properties would be expected in this family. As we have known, the ideal ABO3-typ…     

Fe3O4和Zn2+掺杂型Zn1-xFe2+xO4纳米晶的溶剂热合成和电磁性能

利用溶剂热法, 在醋酸钠静电保护剂的辅助下, 成功制备出Fe₃O₄和Zn²⁺掺杂型Zn_0.07Fe_2.93O₄纳米晶. 利用X射线衍射仪和扫描电子显微镜等对样品的晶体结构、粒径、形貌和化学组成进行了分析. 结果表明, 所得纳米晶的粒径均匀, 形貌为球形, 分散度好; Zn_0.07Fe_2.93O₄纳米晶的平均粒径(70 nm)明显小于Fe₃O₄(170 nm). 磁性能测量结果表明, 室温下Zn_0.07Fe_2.93O₄的饱和磁化强度(54.2 A·m²·kg^-1)小于Fe₃O₄ (81.6 A·m²·kg^-1). 利用矢量网络分析仪对样品的电磁性能和吸波性能进行了研究. 结果表明, Zn²⁺掺杂型Zn_0.07Fe_2.93O₄纳米晶的吸波性能优于Fe₃O₄, 前者的最大吸收峰(-19.3 dB)大于后者(-9.8 dB), 且吸收峰低于-10 dB的峰宽达2.5 GHz.     

Eu3+掺杂的Sr2CeO4荧光材料的燃烧法合成及其性能研究

以尿素作燃料,Sr,Ce和Eu的硝酸盐作反应物,采用燃烧法得到了稀土Eu3 掺杂的Sr2CeO4前驱体粉末.将前驱体在一定温度下烧结3 h,合成了红色荧光材料.经过对材料进行X射线衍射(XRD)分析,确定了烧结温度在1050～1200℃时,能够得到纯度较高的产品.用扫描电镜(SEM)观察到样品烧结后的形貌为不规则的椭圆形,粒径范围在1～3 μm之间.样品的发射光谱和激发光谱表明,Eu3 在Sr2CeO4基质中有很高的猝灭浓度(10%,摩尔分数),随着Eu3 掺杂浓度的增加,可以使蓝白光调整到红白光,进而到红光.     

微米级稀土掺杂NaYF_4荧光粉的水热合成及性质研究

以EDTA为螯合剂,采用水热法合成了微米级单掺Pr3+,Nd3+,Sm3+,Eu3+,Er3+等的NaYF4荧光粉材料。通过XRD和SEM观察分析,得出所合成的材料分散性良好,相纯度较高,并认为EDTA在水热熟化过程中,对控制微晶的形貌有很大的作用;分别在各自对应的几个波长光激发或发射下,可观察到较强的激发峰或发射峰,对发光机制进行了初步探讨,基质晶格场的作用导致了一些发射峰的红移或蓝移。     

Effect of Magnetic Carrier NiFe2O4 Nanoparticles on Physicochemical and Catalytic Properties of Magnetically Separable Photocatalyst TiO2/NiFe2O4

A series of magnetically separable photocatalyst TiO₂/NiFe₂O₄(TN) with different mass ratios of NiFe₂O₄ to TiO₂ was prepared by sol-gel method. The X-ray diffraction(XRD), X-ray photoelectron spectroscopy(XPS), transmission electron microscopy(TEM), ultraviolet-visible spectroscopy(UV-Vis), Brunauer-Emmett-Teller(BET) surface analysis and photoluminescence spectroscopy(PL) were used to characterize the photocatalyst TN. The XRD patterns of TN indicate that adulterating a smidgen of NiFe₂O₄ into TiO₂(about 0.1%, mass ratio) can promote the phase transformation of TiO₂, however, when the doped amount of NiFe₂O₄ surpasses 1%, the introduction of NiFe₂O₄ can inhibit the growth of TiO₂ crystal grain and reduce the size of TiO₂ crystal grain. The XPS results of TN indicate that some Fe³⁺ replace Ti⁴⁺ of the TiO₂ lattice forming Fe―O―Ti bonds. The PL analysis of TN shows that the NiFe₂O₄ nanoparticles in photocatalyst TN play the role of the effective recombination centre of the photogenerated electrons and holes, leading to the decrease in photocatalytic activity.     

Density Functional Theory Approach to the Vibrational Properties and Magnetic Specific Heat of the Covalent Chain Antiferromagnet KFeS2

Ternary potassium-iron sulfide, KFeS₂, belongs to the family of highly anisotropic quasi-one-dimensional antiferromagnets with unusual “anti-Curie–Weiss” susceptibility, quasi-linearly growing with a rising temperature up to 700 K, an almost vanishing magnetic contribution to the specific heat, drastically reduced magnetic moment, etc. While some of the measurements can be satisfactorily described, the deficiency of the entropy changes upon the magnetic transition and the spin state of the iron ion remains a challenge for the further understanding of magnetism. In this work, high-quality single-crystalline samples of KFeS₂ were grown by the Bridgman method, and their stoichiometry, crystal structure, and absence of alien magnetic phases were checked, utilizing wave-length dispersive X-ray electron-probe microanalysis, powder X-ray diffraction, and ⁵⁷Fe Mössbauer spectroscopy, respectively. An ab initio approach was developed to calculate the thermodynamic properties of KFeS₂. The element-specific phonon modes and their density of states (PDOS) were calculated applying the density functional theory in the DFT + U version, which explicitly takes into account the on-site Coulomb repulsion U of electrons and their exchange interaction J. The necessary calibration of the frequency scale was carried out by comparison with the experimental iron PDOS derived from the inelastic nuclear scattering experiment. The infrared absorption measurements confirmed the presence of two high-frequency peaks consistent with the calculated PDOS. The calibrated PDOS allowed the calculation of the lattice contribution to the specific heat of KFeS₂ by direct summation over the phonon modes without approximations and adjustable parameters. The temperature-dependent magnetic specific heat evaluated by subtraction of the calculated phonon contribution from the experimental specific heat provides a lower boundary for estimating the reduced spin state of the iron ion.     

Structural and Magnetic Properties of Bi(Fe1-xMnx)O3

Bi(Fe_1-xMnx)O₃ bulk ceramics with Mn concentration x up to 0.3 were prepared by rapid sintering using sol-gel derived fine powders. Structure transformation is found to depend on the Mn doping concentration by X-ray diffraction and Raman spectroscopy. Bi(Fe_1-xMnx)O₃ maintains the rhombohedral structure of BiFeO3 with x=0.05 and 0.1, but changes to the orthorhombic structure with x=0.3. Weak ferromagnetism is observed for Bi(Fe_1-xMnx)O₃ with x=0.05 and 0.1, but stronger paramagnetism is observed for Bi(Fe_1-xMnx)O₃ with x=0.3 indicating a magnetic phase change from antiferromagnetic to paramagnetic with the structure changing from R3c to C222. Two anomalies at 30 and 140 K are observed for Bi(Fe_1-xMnx)O₃ with x=0.05 and 0.1. The anomaly at 30 K is concluded to be related to the freezing of cluster spin glass from dc magnetic memory and relaxation measurements.     

Effect of Structural Properties of Mesoporous Co3O4 Catalysts on Methane Combustion

Highly ordered 2D and 3D-Co₃O₄ catalysts were prepared using SBA-15 and KIT-6 as templates. Nano-Co₃O₄ catalyst was obtained by calcination of cobalt nitrate as a comparison. The BET surface area of nano-Co₃O₄, 2D-Co₃O₄ and 3D-Co₃O₄ catalysts was 16.2, 63.9 and 75.1 m²/g, respectively. All the catalysts were tested for the total combustion of methane and their catalytic performance was in the order of 3D-Co₃O₄(T₉₀=355℃) >2D-Co₃O₄(T₉₀=383℃) >nano-Co₃O₄(T₉₀=455℃). It was also found that the order of the areal specific reaction rates for the combustion of methane followed the same order of total activity. The characterization result demonstrates that enhanced catalytic performance of methane of the 2D-Co₃O₄ and 3D-Co₃O₄ catalysts is due to their pronounced reducibility and abundant active Co3+ species, which was caused by the preferential exposure of {220} crystal planes in 3D-Co₃O₄ and 2D-Co₃O₄ catalysts compared to the nano-Co₃O₄.     

First Principle Calculation of Electric and Magnetic Properties for New Half-metal Fe2ScO4

The new half-metals Fe2ScO4 and FeSc2O4 were designed and their spinel structures were optimized based on the first-principle pseudo-potential method. Their electric and magnetic properties including molecular magnetic moments and electronic structures were calculated and analyzed, and then were compared with those of Fe3O4. The calculation showed that Fe2ScO4 and FeSc2O4 were both new ferromagnetic II B-type half-metals, but Fe3O4 was ferrimagnetic. The molecular magnetic moment of Fe2ScO4 is about 7.28 1B, which is much larger than the 4.0 1B of Fe3O4 and 3.96 1B of Fe2ScO4. The molecular magnetic moment of Fe2ScO4 mainly came from the spin-polarization of Fe3d electrons. Also, the conductance of Fe2ScO4 was a little larger than that of Fe3O4. For Fe2ScO4, the average electronic structure of Sc on A-sites wasSc+3s23p43d2 and that of Fe on B-sites was Fe2+t2g3↑"tg2↑"t2g↓. It can be predicted that the new half-metal Fe2ScO4 has wider application ground in spin electronic instruments because of its larger magnetoresistance compared to Fe3O4 and FeSc2O4.     

不同浓度Sn4+离子掺杂TiO2的结构、性质和光催化活性

采用溶胶-凝胶法制备出纯TiO₂和不同浓度Sn⁴⁺离子掺杂的TiO₂光催化剂(TiO₂-Snx%, x%代表Sn⁴⁺离子掺杂的TiO₂样品中Sn⁴⁺离子摩尔分数). 利用X 射线衍射(XRD)、X 射线光电子能谱(XPS)和表面光电压谱(SPS)确定了TiO₂-Snx%催化剂的晶相结构和能带结构, 结果表明: 当Sn⁴⁺离子浓度较低时, Sn⁴⁺离子进入TiO₂晶格, 取代并占据Ti⁴⁺离子的位置, 形成取代式掺杂结构(Ti_1-xSn_xO₂), 其掺杂能级在导带下0.38 eV处; 当Sn⁴⁺离子浓度较高时, 掺入的Sn⁴⁺离子在TiO₂表面生成金红石SnO₂, 形成TiO₂和SnO₂复合结构(TiO₂/SnO₂), SnO₂的导带位于TiO₂导带下0.33 eV处. 利用瞬态光电压谱和荧光光谱研究了TiO₂-Snx%催化剂光生载流子的分离和复合的动力学过程, 结果表明, Sn⁴⁺离子掺杂能级和表面SnO₂能带存在促进光生载流子的分离, 有效地抑制了光生电子与空穴的复合; 然而, Sn⁴⁺离子掺杂能级能更有效地增加光生电子的分离寿命, 提高了光生载流子的分离效率, 从而揭示了TiO₂-Snx%催化剂的光催化机理.     

高密度发光材料BiTaO4∶Pr3+和BiTaO4的发光特性研究

研究了BiTaO4∶Pr3+, BiTaO4的光致发光性质, 测量了BiTaO4的红外透射和漫反射光谱. BiTaO4的光致发光光谱发射峰位于约420, 440, 465 nm; 其激发谱在约330～370 nm范围有明显的激发. BiTaO4∶Pr3+的光致发光光谱为Pr3+的特征发射, 主峰为606 nm, 来自Pr3+的3P0→3H6跃迁; 其激发谱由来自于基质的峰值为325 nm和范围在375～430 nm的宽激发带以及Pr3+的特征激发组成, 325 nm, 375～430 nm的激发带可能分别来自钽酸根团的电荷迁移跃迁和基质的带间缺陷能级的吸收; 在BiTaO4∶Pr3+中存在着基质→Pr3+的能量传递. 由于BiTaO4∶Pr3+基质的密度和Pr3+的发光强度均超过PbWO4, 因此BiTaO4∶Pr3+可能是潜在的重闪烁体.     

新型荧光粉Ca2Zn4Ti16O38∶Pr3+，Na+的合成和红色长余辉性质

采用溶胶-凝胶法合成了Ca2Zn4Ti16O38:Pr3+,Na+荧光粉.通过X-射线衍射和荧光光谱表征样品的物相组成和发光性质.X射线衍射(XRD)分析表明添加适量的H3BO3作助熔剂有利于形成良好的Ca2Zn4Ti16O38晶体结构.荧光光谱表明Ca2Zn4Ti16O38:Pr3+,Na+在可见光区(450～495 nm)呈现Pr3+离子的4f→4f厂特征激发光谱以及613 nm(1D2→3H4)和644 nm(3P0→3F2)特征发射.Ca2Zn4Ti16O38:Pr3+,Na+被可见光(475 nm)激发产生的(3P0→3F2)(644 nm)红色发射呈现出极慢的衰减特性.Ca2Zn4Ti16O38:Pr3+,Na+是一种新型的可见光激发红色长余辉荧光粉.     

Effect of VO43- Substitution on the Electrochemical Properties of a LiSn2(PO4)3 Anode Material

VO₄^3- anion was used to partially substitute for PO₄^3- in the Nasicon compound of LiSn₂(PO₄)₃ via a sol-gel method. XRD analysis revealed that the VO₄^3--substituted samples did not have a single LiSn₂(PO₄)₃ phase, and some secondary phases like SnO₂ and SnP₂O₇ appeared. Introduction of the VO₄^3- anion did not prevent the LiSn₂(PO₄)₃ compound from decomposing during the initial lithiation; however the VO₄^3- anion substitution remar-kably enhanced the rate capability and cycling performance of the products because they reduced the charge transfer impedance, increased the lithium ion diffusion, and strengthened the role of the Li₃PO₄ matrix due to the precipitation of the Li₃VO₄phase. Of the substituted samples, the sample with a nominal composition of LiSn₂(PO₄)_2.5(VO₄)_0.5 delivered a capacity of 449.2 mA·h/g at a rate of 0.25 C after 25 cycles and 373.8 mA·h/g at 2 C rate. Those values surpassed some previous reports on LiSn₂(PO₄)₃ and the LiSn₂(PO₄)₃/C composites. Accordingly, the partial substitution of phosphorus by vanadium in LiSn₂(PO₄)₃ is a feasible technique to remarkably improve its electrochemical properties.     

纳米SrAl2O4:Eu2+,Dy3+长余辉发光材料的制备与性能

采用水热-均匀共沉淀法制备了纳米SrAl2O4:Eu2+,Dy3+长余辉发光材料.通过XRD、TEM、荧光光谱、热释光谱对其结构和性能进行分析.XRD结果表明所制备的SrAl2O4:Eu2+Dy3+纳米发光材料为单相,属单斜晶系.TEM测试表明纳米SrAl2O4:Eu2+,Dy3+发光材料为规则的球状粒子,粒径为50～80 nm,且分散性良好.激发和发射光谱测试表明,样品的激发光谱是峰值在356 nm 的连续宽带谱,发射光谱是峰值位于512 nm的宽带谱,与SrAl2O4:Eu2+,Dy3+粗晶材料相比,激发和发射光谱都出现了"蓝移"现象.样品的热释光峰值位于358 K,适合于产生长余辉.     

铈对ZZn4-1锌合金性能和微观组织的影响

在ＺＺｎ４ － １ 锌合金中添加微量铈, 能使其金属模铸造条件下的抗拉强度及布氏硬度有较大提高, 并能有效地改善其微观组织、细化晶粒。在压铸条件下, 添加铈后, 能使压铸件微观组织中无论是初生的η相或共晶相均比没有添加铈的合金细小、弥散、均匀, 从而使其力学性能及工艺性能得到提高, 成品合格率大幅度增加。     

Growth and Spectral Properties of Nd^3＋ Doped KLa（MoO4）2 Crystal

1 INTRODUCTION There has been an increasing interest in the re- search of diode-pumped solid-state lasers in recent years because of the rapid development of high power diode lasers. The absorption peak of Nd3 ions at about 800 nm corresponding to 4I9/2→ 2H9/2 tran- sition is suitable for commercial laser diode GaAlAs pumping[1]. KLa(MoO4)2 is a kind of disordered crystalline host for lasing rare-earth ions[2], and it belongs to Scheelite (CaWO4) structure[3]. The disorder derives…     

银掺杂对CdFe2 O4电导和气敏性能的影响

用溶胶-凝胶法制备了CdFe2O4及其掺银纳米粉,并对其制备条件、物相组成、微结构、电导和气敏性能作了系统研究.结果表明: 350℃下预烧2 h进一步除尽残存柠檬酸的凝胶粉于800℃下热处理2 h可得纯相掺银纳米粉Cd1-xAgxFe2O4(0 ≤x≤0.04); 电导测量显示,该材料呈表面电阻控制的n型半导体导电行为,由于AgCd×电离出的空穴h对材料中导带自由电子的湮灭,使得掺银固溶体的导电性远小于同温下的纯相CdFe2O4; Cd0.98Ag0.02Fe2O4纳米粉制作的元件在330℃下对45 μmol/L C2H5OH的灵敏度为相同浓度干扰气体Petrol的11倍多.有望开发为一类新型C2H5OH信息敏感材料.     

[Ru(bpy)_2tpphz]~(2+)与Zn~(2+)形成的双核配合物的荧光性质研究

近年来,钌多吡啶配合物与DNA的作用得到了比较广泛的研究,并且发展了一系列具有特定功能的钌配合物犤1犦。如传统的DNA分子光开关犤Ru(bpy)2dppz犦2+和犤Ru(phen)2dppz犦2+犤2,3犦(bpy=2,2'-联吡啶,phen=1,10-菲咯啉,dppz=二吡啶犤3,2-a:2',3'-c犦吩嗪)。这些配合物与DNA具有较强的结合力,在水溶液中几乎不发光,但在DNA存在下则有强烈荧光发出。这是由于配合物插入DNA的碱基对之后,保护了dppz的吡嗪环上的N原子,使其免受水分子的进攻从而导致配合物荧光的恢复。但是对于大多数的多吡啶钌配合物来讲,由于其自身较强的背景荧光或与DN…