Synthesis of Magnetic Nickel Ferrite Microspheres and Their Microwave Absorbing Properties

NiFe₂O₄ microspheres were synthesized using a solvothermal method. The morphologies and structures of NiFe₂O₄ micropheres were characterized via a field emission scanning electron microscope(FESEM), a transmission electron microscope(TEM) and an X-ray diffractometer(XRD). The NiFe₂O₄ microspheres were around 150-200 nm in diameter and assembled by nanoparticles. The magnetic and electromagnetic parameters were measured using a vibrating sample magnetometer and a vector network analyzer, respectively. The obtained products exhibited a saturation magnetization of 60.8 A·m²·kg^-1 at room temperature. A minimum reflection loss(RL) of -27.8 dB was observed at 9.2 GHz with a thickness of 3.5 mm, and the effective absorption frequency(RL<-10 dB) ranged from 8.2 GHz to 11.2 GHz, indicating the excellent microwave absorption performance of the NiFe₂O₄ microspheres in the X-band frequencies.     

Structure and Magnetic Properties of Nickel–Zinc Ferrite Nanoparticles Prepared by Glass Crystallization Method

Summary. The magnetic and microstructure properties of Fe₂O₃–0.4NiO–0.6ZnO–B₂O₃ glass system, which was subjected to heat treatment in order to induce a magnetic crystalline phase (Ni_0.4Zn_0.6-Fe₂O₄ crystals) within the glass matrix, were investigated. DSC measurement was performed to reveal the crystallization temperature of the prepared glass sample. The obtained samples, produced by heat treatment at 765°C for various times (1, 1.5, 2, and 3 h), were characterized by X-ray diffraction, IR spectra, transmission electron microscopy, and vibrating sample magnetometer. The results indicated the formation of spinel Ni–Zn ferrite in the glass matrix. Particles of the ferrite with sizes ranging from 28 to 120 nm depending on the sintering time were observed. The coercivity values for different heat-treatment samples were found to be in the range from 15.2 to 100 Oe. The combination of zinc content and sintering times leads to samples with saturation magnetization ranging from 12.25 to 17.82 emu/g.     

静电纺丝法制备铁酸锌中空纤维及其磁学性能

以锌盐、铁盐和聚乙烯吡咯烷酮(PVP)为原料,通过静电纺丝法先制备PVP/硝酸盐复合纤维,这些复合纤维以5℃·min-1的升温速率加热到500℃并保温3h,最终得到铁酸锌(ZnFe2O4)中空纤维.通过X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)以及振动样品磁强计(VSM)等分析手段对中空纤维的晶体结构、形貌和磁学性能进行了研究.结果显示,ZnFe2O4中空纤维属于尖晶石结构,高温处理后仍能保持一维结构,纤维直径在200-400nm之间,纤维壁由大小为25nm的颗粒堆积而成.室温磁化结果显示制备的ZnFe2O4中空纤维具有超顺磁性,在10kOe的磁化强度为2.03emu·g-1.     

Structural Transition and Magnetic Property of Bi1-xYbxFeO3

Bi_1-xYb_xFeO₃(0≤x≤0.2) powders have been synthesized using a sol-gel method. The X-ray diffraction data show a structural transition from the rhombohedral R3c phase to the orthorhombic Pnma phase between x=0.1 and 0.125, which should induce a ferroelectric- paraelectric transformation. The phase transition is also proven by the Raman spectroscopy. A moderate signal on magnetization appears to illustrate the enhancement of magnetization at the transformation boundary, which is suggested to be the destruction of the spin cycloid structure at low concentration. The appearance of antiferromagnetic ordering is proposed to account for the afterward reduction of the magnetization at high concentration.     

La-Co共掺杂的M型锶铁氧体纳米纤维的制备和磁性能

以聚乙烯吡咯烷酮(PVP)和金属盐为原料,采用静电纺丝、溶胶-凝胶技术以及随后的热处理工艺,制备了La、Co共掺杂的M型锶铁氧体Sr1-xLaxFe12-xCoxO19(x=0.12)(SLFC)纳米纤维.利用X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)和超导量子干涉仪(SQUID)技术对纳米纤维样品的结构、形貌和磁学性能进行了观测,系统地研究了不同温度下样品的磁性能变化.结果表明:经过950°C焙烧2h后,得到纯相的M型锶铁氧体纳米纤维,纤维呈竹节状结构,直径约55nm;室温下测得矫顽力(Hc)为498.53kA·m-1,饱和磁化强度(Ms)为70.76A·m2·kg-1,剩磁(Mr)为36.35A·m2·kg-1,这比未掺杂SrFe12O19(SF)时纳米纤维的磁性能有明显的改善,并且与在相同温度下制得的相应纳米粉体样品相比,磁性能明显提高.     

Influence of Rare Earth Ho3+ Doping on Structural,Microstructure and Magnetic Properties of ZnO Bulk and Thin Film Systems

We have investigated the doping behavior of rare earth element holmium (Ho³⁺) in ZnO semiconductor. The structural, microstructure, and magnetic properties of Zn_1-xHo_xO (x=0.0, 0.04, and 0.05) thin films deposited on Si(100) substrate by thermal evaporation technique were studied. The ceramic targets were prepared by conventional solid state ceramic technique. The pallets used as target were final sintered at 900 oC in the presence of N2 atmosphere. The experimental results of X-ray diffraction (XRD) spectra, surface morphology, and magnetic properties show that the Ho³⁺ doped ZnO thin films has a strong influence on the materials properties. The higher angle shift in peak position and most preferred (101) orientation were observed in XRD pattern. These spectra confirmed the substitution of Ho3+ in ZnO lattice. The surface morphology and stoichiometry for both bulk and thin films were analyzed by scanning electron microscopy and energy dispersive spectroscopy. It was observed that grain size decreases with the increase of Ho³⁺. Room temperature ferromagnetism was observed for Zn_0.95Ho_0.05O films. The ferromagnetism might be attributed to the substitution of Ho ions for Zn²⁺ in ZnO lattices.     

聚丙烯酸酯-LiNi铁氧体纳米复合物的制备和磁性研究

用流变相法制备了LiNi铁氧体纳米粒子, 通过硅烷偶联剂对纳米LiNi铁氧体表面改性, 用乳液聚合法制备了纳米LiNi铁氧体-聚丙烯酸酯复合物. 用X射线衍射(XRD)、红外光谱(IR)、透射电镜(TEM)、热重分析(TGA)、振动样品磁强计(VSM)以及阻抗-材料分析仪等表征了样品的结构、形貌和磁性能. 结果表明, 引入的纳米铁氧体被聚丙烯酸酯分子链所包覆, 明显提高了复合物的热稳定性. 在外加磁场下, 复合物表现出了较弱的亚铁磁性, 并具有一定的磁滞损耗特性.     

溶胶-凝胶法制备单磁畴m型六角钡铁氧体及磁性

sol-gel法;钡铁氧体;单磁畴;磁性     

添加Al、Mg、W、Mo对烧结Nd-Fe-B磁体磁性能与显微组织的影响

研究了在烧结ＮｄＦｅＢ磁体晶间添加Ａｌ、Ｍｇ、Ｗ、Ｍｏ等合金元素对显微组织和磁性能的影响。实验结果表明：低熔点合金元素Ａｌ、Ｍｇ能显著提高ＮｄＦｅＢ磁体的矫顽力，略微降低剩磁，对磁体的热稳定性无影响；高熔点合金元素Ｗ、Ｍｏ在不降低剩磁的情况下亦能提高磁体的矫顽力，但效果不如Ａｌ、Ｍｇ明显。显微组织分析表明，在添加低熔点和高熔点合金元素的磁体晶间发现了两种不同的新相。矫顽力的提高可归于晶间新相的出现。进一步分析表明，与传统的合金化相比，对ＮｄＦｅＢ磁体晶间区域进行微合金化是改进ＮｄＦｅＢ磁体组织与性能的一种更为有效的手段。     

Mn0.6 Zn0.4 Fe2 O4 磁性亚微球的可控合成及磁性能

采用溶剂热法制备了单分散Mn0.6Zn0.4Fe2O4磁性亚微米球, 研究了反应工艺参数对磁性亚微米球结构形貌、 直径和静磁性能的影响规律. 研究发现, 随着反应时间的延长, 体系中的金属离子首先水解沉淀, 形成羟基氧化铁及Mn, Zn氢氧化物, 然后脱水转化为Mn0.6Zn0.4Fe2O4球形纳米粒子, 这些纳米粒子发生团聚, 形成结构疏松、 大小不均匀的亚微米粒子, 最后通过Ostwald熟化过程, 形成致密的单分散亚微米球. 降低反应溶液的pH值、 增加乙二醇或聚乙二醇的用量, 均会使亚微球的直径增大, 并可在150~500 nm范围内调控微球的粒径; 但组成磁性亚微球的纳米粒子的粒径逐渐减小, 产物的饱和磁化强度增大, 矫顽力和剩磁减小.     

镝掺杂铁氧体纳米晶的制备、表征和磁性

采用化学共沉淀法制备出了镝掺杂铁氧体纳米晶, 利用透射电子显微镜(TEM)、X射线衍射仪(XRD)、傅立叶红外光谱仪(FTIR)、古埃磁天平、振动样品磁强计(VSM)、X射线能谱仪(EDX)等仪器对产物进行了表征, 研究了Dy^3＋掺杂量对铁氧体纳米晶的结构、磁性和粒度的影响. 结果表明: 适量稀土元素镝离子的掺杂可以提高尖晶石型铁氧体的磁性、降低矫顽力, 当n(Fe^3＋)∶n(Dy^3＋)＝14∶1时其磁性最强. Dy^3＋替代或充填进入了尖晶石晶格, 且主要占据B位. 掺杂了镝的铁氧体磁性纳米粒子粒度变小, 且分布更集中、均匀, 当Dy^3＋加入量为n(Fe^3＋)∶n(Dy^3＋)＝14∶1时铁氧体纳米粒子的平均粒径由掺杂前的14 nm降低到到8 nm. 这种具有超顺磁性的软磁铁氧体纳米晶可应用于纳米磁液领域.     

The Electronic and Magnetic Properties of a Few Transition-Metal Clusters

Using density functional theory we present a systematic study of the electronic and magnetic properties of various nickel clusters and two small bimetallic clusters, Ni _n Co _m and Ni _n Fe _m (n + m ≤ 6). A detail study of binding energy, magnetic moment and stability function of pure nickel clusters of nuclearity (N) 40–60 have been performed. We observe that the magic numbers occur at N = 43, 46, 49, 53, 55, and 58, which correspond to the most stable clusters. We find that, with increase in substitution of Co and Fe atoms in Ni cluster, while Ni _n Co _m becomes more stable, the Ni _n Fe _m clusters become less stable. The significant enhancement of average magnetic moment and suppression of local magnetic moment of nickel atoms are found in both clusters with increase in Co and Fe concentration.     

Structural and Magnetic Properties of Chemically Synthesized Pd-Modified NiFe2O4 Nanoparticles

Magnetic nanoparticles of NiFe₂O₄-Pd composites have been synthesized using a simple, low cost, sol-gel auto-combustion method. As-prepared samples were sintered at 800 ℃ for 6 h in order to develop the crystalline phase. X-ray diffraction confirmed the spinel structure of the ferrite samples. Structural morphology and size of the nanoparticles were evaluated using a field emission scanning electron microscope. Magnetic hysteresis loops were obtained at 300 and 100 K using a physical properties measurement system. The value of saturation magnetization was observed to decrease at the temperatures with the increase of Pd contents up to 5% but then a sudden rise in saturation magnetization was observed for the addition of 10% Pd in NiFe₂O₄.     

Preparation, Characterization and Magnetic Properties of PANI/La-substituted LiNi Ferrite Nanocomposites

Magnetic nanocomposites containing polyaniline （PANI）-coated La-substituted LiNi ferrite （LiNi0.5La0.02Fe1.98O4） were synthesized by in situ polymerization in aqueous solution of hydrochloric acid. The nanocomposites exhibited the magnetic hysteresis nature under applied magnetic field. The saturation magnetization （Ms） and coercivity （Hc） varied with the ferrite content. The obtained nanocomposites were characterized by X-ray diffraction （XRD）, transmission electron microscopy （TEM）, scanning electron microscopy （SEM）, Fourier transform infrared spectroscopy （FT-IR）, UV-Visible spectroscopy and vibrating sample magnetometer （VSM）. TEM and SEM studies showed that the nanocomposites present the core-shell structure. The results of XRD patterns, FT-IR and UV-Visible spectra indicated the formation of PANI-LiNi0.5La0.002Fe1.98O4 nanocomposites and showed that the interaction existed between PANI backbone and ferrite particles in the nanocomposites. The bonding mechanism in the nanocomposites has been proposed.     

Ge_nEu(n=1-13)团簇的结构、电子及磁性质(英文)

利用密度泛函理论在广义梯度近似下研究了GenEu(n=1-13)团簇的生长模式和磁性.结果表明:对于GenEu(n=1-13)团簇的基态结构而言,没有Eu原子陷入笼中.这和SinEu以及其它过渡金属掺杂半导体团簇的生长模式不同.除GeEu团簇外,GenEu(n=2-13)团簇的磁矩均为7μB.团簇的总磁矩与Eu原子的4f轨道磁矩基本相等.Ge、Eu原子间的电荷转移以及Eu原子的5d、6p和6s间的轨道杂化可以增强Eu原子的局域磁矩,却不能增强团簇总磁矩.     

热处理条件对BaSm0.3Fe11.7O19铁氧体纤维结构演化和磁性能的影响

以金属盐和柠檬酸为原料,采用溶胶凝胶法成功制备1μm以下具有较大长径比的纳米晶BaSm0.3Fe11.7O19 铁氧体纤维。采用热重-差热分析(TG-DSC)、X射线衍射仪(XRD)、场发射扫描电镜(FE-SEM)和振动样品磁强计(VSM)对前躯体纤维及其焙烧产物进行了表征。实验结果表明,750℃焙烧1小时,BaSm0.3Fe11.7O19铁氧体相已基本形成,随着焙烧温度的升高和保温时间的延长,BaSm0.3Fe11.7O19晶粒尺寸逐渐增大,纤维表面越发粗糙,片状结构越发明显。同时,纤维的饱和磁化强度(Ms)随晶粒尺寸的增加而增大,而矫顽力(Hc)则呈现先增大后减小的趋势,在晶粒尺寸为58.4 nm附近达到最大值459.2 kA/m,这表明Sm0.3Fe11.7O19纤维的临界单畴尺寸在60nm左右。对低温(77K)和室温(300K)样品的磁性能比较发现,磁性能存在明显的差异,这主要与纳米晶的表面自旋有关。     

Structural,Magnetic and Optical Properties of BiFe1-xNbxO3

Nb doped multiferroic BiFe_1-xNb_xO₃ (0 <x <0.05) polycrystalline powders have been syn-thesized by using a sol-gel method. The effect of Nb dopant on the structural, magnetic and optical properties is investigated. According to the X-ray di raction data and the result of Rietveld re nement, all the samples maintain the R3c phase, while the lattice parameters a, c, the cell volume V and the Fe-O-Fe bond angle change. The remnant magnetization enhances by appropriate Nb doping due to the decreasing of the grain size. Meanwhile, Nb dopant leads to the narrowing of the band gap of BiFe_1-xNb_xO₃ samples.     

Structure and Magnetic Properties of Nickel–Zinc Ferrite Nanoparticles Prepared by Glass Crystallization Method

The magnetic and microstructure properties of Fe₂O₃–0.4NiO–0.6ZnO–B₂O₃ glass system, which was subjected to heat treatment in order to induce a magnetic crystalline phase (Ni_0.4Zn_0.6-Fe₂O₄ crystals) within the glass matrix, were investigated. DSC measurement was performed to reveal the crystallization temperature of the prepared glass sample. The obtained samples, produced by heat treatment at 765°C for various times (1, 1.5, 2, and 3 h), were characterized by X-ray diffraction, IR spectra, transmission electron microscopy, and vibrating sample magnetometer. The results indicated the formation of spinel Ni–Zn ferrite in the glass matrix. Particles of the ferrite with sizes ranging from 28 to 120 nm depending on the sintering time were observed. The coercivity values for different heat-treatment samples were found to be in the range from 15.2 to 100 Oe. The combination of zinc content and sintering times leads to samples with saturation magnetization ranging from 12.25 to 17.82 emu/g.     

钐掺杂对锰锌铁氧体微波电磁性能的影响

采用同相法合成了钐掺杂的锰锌铁氧体Mn0.3Zn0.7Fe2-xSmxO4,(x=0,0.01,0.02,0.04,0.06),通过XRD对合成粉末进行了晶体结构的分析,结果表明:当x≤0.02时,制得的粉体为相对较纯的尖品石型铁氧体.稀土掺杂锰锌铁氧体的晶格常数随着掺钐量的增加先增大后减少.使用Agilent8722ET网络分析仪在2～18 GHz的频率范围内对其微波电磁特性进行测试,结果显示,当掺钐量为0.02时,在9～18 GHz的频率范围内电磁参数ε'和ε"稍有增加,ε"最大值出现的位置移向低频.μ"和μ'峰值均大大增加,最大值分别达到6.2和5.5,该掺钐晕下微波电磁性能最佳.利用微波电磁理论分析了电磁参数的变化机制.     

不同结构CoPt纳米棒磁学性能

运用电位置换结合化学还原方法制备了两种不同结构的CoPt纳米棒材料,一种为实心结构(CoPt-a),一种为空心结构(CoPt-b).采用透射电镜(TEM)和能量散射光谱(EDS)研究了其形貌和组成.在5和300K下测试了两种纳米棒的磁学性能.结果显示,CoPt-a和CoPt-b纳米棒在5K时的矫顽力分别为6.5和9.3A·m-1,温度升至300K时,两种结构CoPt纳米棒矫顽力均减小为0A·m-1.场冷曲线(FC)和零场冷曲线(ZFC)结果表明两种结构的CoPt纳米棒均表现出超顺磁性,阻塞温度(TB)分别为10.0和9.0K.两种CoPt纳米棒组成、结构等不同可能是引起其矫顽力、磁化强度和阻塞温度差异的主要原因.