In-situ synthesis of magnetic (NiFe2O4/CuO/FeO) nanocomposites

In-situ synthesis of magnetic nanocomposites with (NiFe₂O₄/CuO/FeO) crystal phases has been done using a sol-gel method by taking a non-stoichiometric composition of the precursors. The average particle size of the nanocomposites was calculated using X-ray diffraction (XRD) and high resolution tunneling electron microscope (HR-TEM) and it turns out to be ∼20 nm. The vibrating sample magnetometer (VSM) measurements demonstrate the ferromagnetic nature of the nanocomposites. The synthesized nanocomposite was used to prepare magnetic fluid using tetramethylammonium hydroxide as a surfactant and its stability in the solution was also discussed.     

NiFe2O4磁性纳米材料的溶剂热法一步合成

以Fe(NO_3)_3·9H_2O和Ni(NO_3)_2·6H_2O为原料,在未添加任何碱性沉淀剂和高温晶化处理的条件下,通过对实验条件(包括溶剂、溶剂热温度和时间)的优化,利用溶剂热法一步制备了具有良好结晶性和超顺磁性的NiFe_2O_4磁性纳米材料。结果表明:用H_2O和EtOH-H_2O做溶剂都不利于NiFe_2O_4的生成;用EtOH做溶剂,为了获得纯度较高的NiFe_2O_4磁性纳米材料,要保证适当的溶剂热温度和时间;所得材料的磁性能与材料中磁性组分NiFe_2O_4的含量和其结晶程度有关。该制备方法最突出的优点是简单、快速、成本低、从源头消除了污染,且所得的材料磁性能优良。     

尖晶石结构MFe2O4(M=Ca,Mg,Cu,Zn)纳米晶粉末的制备和磁性能

采用新型氨基凝胶自燃法成功制备出尖晶石结构MFe₂O₄（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MFe₂O₄粉末的高纯度。系统地研究了所合成的MFe₂O₄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CaFe₂O₄和MgFe₂O₄两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CaFe₂O₄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。     

复合多铁材料NiFe2O4/BaTiO3的制备及性能

采用溶胶-凝胶与固相反应相结合的方法制备了xNiFe2O4/(1-x)BaTiO3(x=0.1,0.2,0.3,0.4,0.5,0.6)系列复合多铁材料.X射线衍射(XRD)结果表明,复合材料中只含有钙钛矿结构的BaTiO3和尖晶石结构的NiFe2O4,说明共烧过程中两者未发生明显的化学反应,铁电相与铁磁相共存.扫描电子显微镜(SEM)观测结果表明材料内部是异质结构的,高分辨透射电子显微镜(HRTEM)观测结果进一步说明了NiFe2 O4和BaTiO3共存,并且在两种物质的接触处能够看到清晰的界面.这种由BaTiO3和NiFe2 O4组成的复合材料对外同时表现出铁电性和铁磁性.电滞回线结果表明,该复合材料具有铁电性,但存在着一定的漏电.介电频谱表明材料的介电常数随着频率的升高而下降,在低频下达到定值,并且铁磁相的含量对材料的介电性有影响.磁性能测试结果表明材料的磁性源于NiFe2O4,并且磁性随着NiFe2O4含量的增加而增强.     

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.     

一种便捷方法制备表面氨基化的超顺磁Fe3O4纳米粒子

提出了一种简便易行的对磁性纳米粒子表面进行氨基化的方法. 首先使用化学共沉淀法合成了粒径为10 nm左右的Fe3O4纳米粒子, 然后用阿仑膦酸钠对其表面进行修饰, 使其表面具有了功能化的氨基. 利用透射电子显微镜(TEM)、X射线衍射(XRD)、振动样品磁强计(VSM)、动态光散射(DLS)仪、热重分析(TGA)仪、傅里叶变换红外(FT-IR)光谱仪、X射线光电子能谱(XPS)仪等对其进行表征. 结果显示磁性纳米粒子表面被成功地修饰了一层双膦酸分子. 所制备的纳米粒子可在pH=6.3稳定存在4周以上.     

氨基化修饰介孔Fe3O4@SiO2@mSiO2磁性核壳复合微球的可控制备及吸附性能

以水热法制备的高磁饱和强度Fe₃O₄纳米颗粒为核,正硅酸乙酯（TEOS）为前驱体,采用改进的Stöber法,制备介孔SiO₂包覆Fe₃O₄磁性核壳复合微球。利用XRD、SEM、TEM、N₂吸-脱附、FTIR和VSM对制备样品的物相结构、形貌和磁性能进行了测试表征。研究结果表明,制备的复合材料呈球形,粒径分布均一,材料的比表面积和磁饱和强度分别为413 m²·g^-1和68.93 emu·g^-1。研究了TEOS的添加量对复合微球形貌的影响,随着TEOS添加量的增加,SiO₂壳层增厚,复合粒子形貌均匀,饱和磁化强度有所下降,仍具有良好的超顺磁性。在此基础上,通过接枝法在复合微球的表面接枝-NH₂,制备了一种新型磁性纳米吸附剂（Fe₃O₄@SiO₂@mSiO₂-NH₂）,进而研究了其对水中重金属离子Cr（Ⅳ）的吸附性能。通过动力学拟合,Fe₃O₄@SiO₂@mSiO₂-NH₂对Cr（Ⅳ）的吸附过程是准二级动力学模型占主导地位。探究了该材料对Cr（Ⅳ）的吸附过程和吸附机理。结果表明,其吸附机理及吸附容量与Cr（Ⅳ）的离子形态及-NH₂有关,并通过吸附剂与吸附质之间的电子共用或静电吸附实现。     

氨基化修饰介孔Fe3O4@SiO2@mSiO2磁性核壳复合微球的可控制备及吸附性能

以水热法制备的高磁饱和强度Fe_3O_4纳米颗粒为核,正硅酸乙酯(TEOS)为前驱体,采用改进的St觟ber法,制备介孔SiO_2包覆Fe_3O_4磁性核壳复合微球。利用XRD、SEM、TEM、N2吸附-脱附、FTIR和VSM对制备样品的物相结构、形貌和磁性能进行了测试表征。研究结果表明,制备的复合材料呈球形,粒径分布均一,材料的比表面积和磁饱和强度分别为413 m2·g-1和68.93emu·g-1。研究了TEOS的添加量对复合微球形貌的影响,随着TEOS添加量的增加,SiO_2壳层增厚,复合粒子形貌均匀,饱和磁化强度有所下降,仍具有良好的超顺磁性。在此基础上,通过接枝法在复合微球的表面接枝-NH2,制备了一种新型磁性纳米吸附剂(Fe_3O_4@SiO_2@m SiO_2-NH2),进而研究了其对水中重金属离子Cr(Ⅵ)的吸附性能。通过动力学拟合,Fe_3O_4@SiO_2@m SiO_2-NH2对Cr(Ⅵ)的吸附过程是准二级动力学模型占主导地位,探究了该材料对Cr(Ⅵ)的吸附过程和吸附机理。结果表明,其吸附机理及吸附容量与Cr(Ⅵ)的离子形态及-NH2有关,并通过吸附剂与吸附质之间的电子共用或静电吸附实现。     

叶酸对磁性Fe_3O_4纳米粒子的表面修饰

以FeCl3·6H2O作为单一铁源,1,6-己二胺作为胺化试剂,利用无模板的溶剂热方法制备了胺基功能化的磁性Fe3O4纳米粒子,并利用其键合叶酸分子,制备出表面修饰了叶酸的磁性Fe3O4复合纳米粒子。利用傅里叶变换红外光谱仪、X-射线衍射仪、透射电镜、差热-热重分析仪和振动样品磁强计对所得纳米粒子的形貌、粒径、化学组成和磁性能进行了表征。结果表明,叶酸分子通过化学键牢固键合在磁性纳米Fe3O4粒子表面,叶酸修饰的复合纳米粒子仍然具有良好的磁性能。     

静电纺丝法制备的钴酸镍微米带的磁性以及电化学性能

通过直接退火静电纺丝前驱样品以及调节升温速率最终得到了钴酸镍(NiCo₂O₄)微米带. 通过X射线衍射、扫描电镜、振动样品磁强计以及电化学工作站等分析手段对钴酸镍微米带的晶体结构、形貌、磁学性能以及电化学性能进行了研究. 结果显示, 以1℃·min^-1的升温速率得到的NiCo₂O₄微米带属于立方尖晶石结构, 高温处理后仍能保持一维结构. 室温磁化结果显示制备的NiCo₂O₄微米带具有超顺磁性, 在10 kOe时磁化强度为6.35 emu·g^-1. 此外, 电化学测试结果显示, NiCo₂O₄微米带的电容特性是典型的赝电容, 并且比电容随着放电电流密度的增加而减小.     

可控粒径纳米Fe_3O_4的制备及其磁性研究

本文用空气氧化法,在可见光作用下,添加配合剂(EDTA、柠檬酸、酒石酸、谷氨酸)在室温进行了不同粒径纳米Fe3O4的制备及其磁性能研究。结果表明:在可见光作用下,随EDTA、柠檬酸、酒石酸、谷氨酸等配合剂的添加,得到纳米Fe3O4的粒径有所减小、分散性有所提高;配合剂及可见光共存时,体系反应速率得到提高,高的反应速率使纳米Fe3O4晶粒减小;控制适当的光照度和添加剂的量,室温可得到11.8~29.6nm的Fe3O4颗粒。不同粒径纳米Fe3O4分别呈现出超顺磁性、铁磁性特征。     

Fe3O4/N-异丙烯酰胺(PNIPAM)纳米颗粒的合成

A magnetic and thermosensitive poly(N-isopropylacrylamide)(PNIPAM) nanoparticles were prepared by the following procedure. The core-shell composite microparticles were synthesized by precipitating polymerization with Fe₃O₄ being entrapped with SiO₂ as core and cross-linked PNIPAM as shell. Then， the SiO₂ core was etched by hydrofluoric acid and magnetic thermosensitive Fe₃O₄/PNIPAM particles were formed. It has also been shown that the Fe₃O₄/PNIPAM nanoparticles are featured by lower critical solution temperature (LCST) at 33.0 ℃ while the temperature varies from 28.0 ℃ to 36.0 ℃. The composite magnetic thermosensitive particles were characterized by XRD， SEM， TEM and FTIR. The synthetic mechanism is also discussed.     

水溶性Fe3O4磁性纳米催化剂的合成及应用

利用对氨基苯磺酸氟硼酸重氮盐与Fe₃O₄磁性纳米粒子(MNPs)的偶联反应,非常方便地制备出表面含有磺酸基的Fe₃O₄磁性纳米粒子。 透射电子显微镜(TEM) 测试结果表明,粒子的平均粒径在 20 nm左右。 溶解性实验表明,该纳米粒子具有较好的水溶性,但不溶于常用的有机溶剂,因此可利用其磁性回收并循环使用。 将该纳米粒子用于催化羧酸与醇的酯化反应,产物酯的收率为71%~86%。 催化剂在酯化反应中的最优使用量为1.5%(质量分数)。 同时,该催化剂可催化果糖合成5-羟甲基糠醛(HMF),收率为32%。     

Fe3O4磁性纳米粒子的超声包金及其表征

超声条件下, 在乙醇分散的3-氨丙基三乙氧基硅烷(APTES)功能化的磁性Fe₃O₄纳米粒子和四氯合金酸的混合溶液中滴加柠檬酸钠, 成功地制备了磁性Fe₃O₄/Au复合纳米粒子. 采用X射线粉末衍射仪(XRD)、紫外吸收可见光谱(UV-Vis)、带有电子能谱仪(EDS)的扫描电子显微镜(SEM)、透射电子显微镜(TEM)、光电子能谱(XPS)、超导量子干涉仪(SQUID)等方法, 对复合粒子的形态、结构、组成以及磁学性质进行了表征. 结果表明: 在此条件下制得的复合粒子粒径在30 nm左右, 室温下磁化强度可达63 emu/g.     

Magnetic properties of Co2V2O7 single crystals grown by flux method

Based on the phase diagram of CoO–V₂O₅ system, single crystals of Co₂V₂O₇ are grown using V₂O₅ as self-flux at a slow cooling rate. The quality of grown crystals is analyzed by X-ray powder diffraction and electron probe microanalysis techniques. Magnetic properties are investigated by means of susceptibility, magnetization, and heat capacity measurements. Our experimental results suggest that Co₂V₂O₇ is a three-dimensional antiferromagnet, in which two magnetic transitions may occur at low temperature and a spin-flop-like transition may occur at the applied field along the b-axis. By contrast to Ni₂V₂O₇, it is suggested that similar and different magnetic properties may arise from their similar crystal structures and different magnetic ions, respectively.     

NiFe2O4/T-ZnOw复合材料的制备及电磁波吸收性能

采用铁氧体化学镀在四角氧化锌晶须(T-ZnOw)表面包覆NiFe2O4镀层,制备了NiFe2O4/T-ZnOw复合材料。利用X射线衍射仪、扫描电镜、能谱分析仪对镀覆前后T-ZnOw的结构、形貌等进行了表征。利用矢量网络分析仪研究了NiFe2O4/T-ZnOw复合材料的电磁波吸收性能。结果表明,化学镀覆后,在T-ZnOw表面包覆了尖晶石型NiFe2O4镀层,生成了NiFe2O4/T-ZnOw复合材料,该材料为磁损耗型材料。化学镀覆过程中T-ZnOw的装载量会影响复合材料的介电常数和磁导率,当T-ZnOw装载量为0.2g时,所制备的复合材料具有最大的介电常数、磁导率、介电损耗和磁损耗,当吸收层厚度达到3 mm时,反射率在14 GHz处达到-11 dB。     

TiO2-CoFe2O4磁性复合材料制备及太阳光催化性能

以四氯化钛、三价铁盐和二价钴盐为前驱体,采用超声波技术一步合成了TiO2-CoFe2O4新型复合光催化剂,运用VSM、XRD、TEM和UV-Vis技术进行了表征,以甲基橙为模拟污染物在太阳光照射下研究其光催化活性。结果表明:所制得的样品具有良好的顺磁性,其饱和磁化强度为212 Gs;样品中TiO2和CoFe2O4分别以锐钛矿相和尖晶石结构存在,粒径尺寸在40～50 nm之间;样品在紫外-可见区有很强的吸收。光催化结果表明复合催化剂具有较高的太阳光催化活性,循环使用3次,仍能保持良好的催化活性。     

A simple route to synthesize nanocrystalline nickel ferrite (NiFe2O4) in the presence of octanoic acid as a surfactant

Nanocrystalline nickel ferrite (NiFe₂O₄) powder was prepared by a co-precipitation method from Ni and Fe chlorides. The as-prepared samples were characterized by powder X-ray diffractometry (XRD), transmission electron microscopy (TEM), scanning electron microscopy (SEM), Fourier transform infrared spectroscopy (FT-IR) and vibrating sample magnetometry (VSM). SEM and TEM indicated that the particles were spherical with particle sizes in the range 25 ± 5 nm. The magnetic properties of the sample were measured by using a vibrating sample magnetometer, which showed that the sample exhibited typical ferromagnetic behavior at room temperature, while a finite coercivity of 245.5 Oe was present at 300 K. The saturation magnetization of the sample (23.13 emu/g) was significantly lower than that for the reported multidomain bulk particles (55 emu/g), reflecting the ultrafine nature of the sample.     

Synthesis and Soft Magnetic Properties of Mg-doped Ni Nanoparticles

Mg-doped Ni nanoparticles with good soft magnetic properties were prepared with the sol-gel method and were sintered at 400, 500, 600, and 900℃ in argon atmosphere, respectively. The structure and magnetic properties of the samples were studied by means of X-ray diffraction, TEM, and VSM magnetometers. X-Ray powder diffraction results show that Ni-Mg solid solution was formed with the single phase of face-centered cubic（fcc） structure. The particle size became larger with the increase of temperature. When the sintering temperature was 400 °C, the particle size was 6.3 nm, whereas it was 46.2 nm at 900 °C. Both the saturation magnetization（Ms） and the coercivity were enhanced with the increase of the particle size. The Ms values of the samples ranged from 18.965 to 46.766 emu/g and the coercivity ranged from 1051.3568 to 9145.0848 A/m.     

Saturation Magnetization and Law of Approach to Saturation for Self-formed Ionic Ferrofluids Based on MnFe2O2 Nanoparticles

The magnetization curves of MnFe₂O₂ nanoparticles and self-formed ferrofluids based on these particles have been measured at room temperature. The median size of the particlesis 13.67 nm. The specific saturation magnetization is less than the theoretical value for theferrofluids. In the high field range from 5 kOe to 10 kOe, the higher the particle volume fraction is, the steeper the slope of the magnetization curves is when it approaches saturation.The behavior of the saturation magnetization and the law of approach to saturation are due to the presence of self-assembled aggregates of ring-like micelle structures which form in the absence of the magnetic field and field-induced aggregates, respectively. The field-induced aggregates have a dissipative structure, so that at high field, the law of approach to saturation magnetization is different from the one described using Langevin paramagnetism theory. The large particles in the ferrofluids result in apparent hysteresis.