Fe_3O_4@SiO_2@CdTe磁性荧光复合微球的制备与表征

采用水热合成法和Stber法制备了氨基功能化SiO2包覆的Fe3O4磁性纳米微球Fe3O4@SiO2-NH2,它与巯基乙酸修饰的CdTe量子点通过酰胺缩合反应,将量子点键合到磁性微球上,制备出单分散性的Fe3O4@SiO2@CdTe磁性荧光双功能微球.用透射电子显微镜、X-射线衍射仪、荧光分光光度计、振动样品磁强计表征了该纳米复合微球的结构和性能.结果表明:Fe3O4@SiO2@CdTe磁性荧光复合微球单分散性好,平均粒径为470nm,饱和磁化强度为37.9emu/g,具有良好的超顺磁性和较高的荧光发光效率.     

简单的方法制备°-Fe2O3纳米粒子及其磁性质和电化学性质

报道了制备磁性Fe2O3纳米粒子的一种简单易行的方法．利用部分还原共沉淀法， 以Na2S2O4作为还原剂， 用FeCl3先制备出Fe2O3纳米微粒， 再在空气中直接煅烧， 成功地制备出粒径较均匀(约13 nm)的磁性Fe2O3微粒． 实验发现Na2S2O4在部分还原共沉淀法中起到了去氧剂兼还原剂的特殊作用．研究表明， 样品在室温下具有铁磁性， 其饱和磁化强度和矫顽力分别为70 emu/g和164 Oe； 产物具有好的电化学性质，在3.0?0.3 V(相对于金属锂)、0.2 mA/cm2时，样品的首次放电容量可达到933 mAh/g．同时还讨论了放电过程中金属锂与Fe2O3的反应机理．     

磁性聚苯胺纳米微球的合成与表征

报道了具有核壳结构的Fe3 O4 聚苯胺磁性纳米微球的合成方法和表征结果 .微球同时具有导电性和磁性能 .在优化的实验条件下 ,可得到饱和磁化强度Ms 为 5 5 .4emu/g ,矫顽力Hc 为 6 2Oe的磁性微球 .微球的导电性随着微球中Fe含量的增加而下降 .微球的磁性能则随着Fe含量的增加而增大 .Fe3 O4 磁流体的粒径和磁性聚苯胺微球的粒径均在纳米量级 .纳米Fe3 O4 粒子能够提高复合物的热性能 .实验表明 ,磁流体和聚苯胺之间可能存在着一定的相互作用 ,但这种相互作用较为复杂 ,难于研究 .     

H2O2氧化法制备Fe3O4纳米颗粒及与共沉淀法制备该样品的比较

在近中性条件下,利用H2O2氧化Fe(OH)2胶体成功制备了Fe3O4纳米颗粒.分别利用透射电镜(TEM),x射线衍射仪(XRD),振动样品磁强计(VSM)和超导量子干涉仪(SQUID)对样品的形貌,结构,宏观磁性进行了表征和测量.TEM图像表明样品为球形颗粒,直径大小约18nm,且分布较均匀.XRD结果表明样品为立方尖晶石结构.穆斯堡尔谱测量表明样品室温下对应两套六线谱,样品的晶体结构存在缺陷,内磁场略小于块体Fe3O4的值.宏观磁测量表明样品的饱和磁化强度可达67×10-3A·m2/g,在20 K出现了Verwey转变.选择该法制备的Fe3O4纳米颗粒与共沉淀法得到的样品作了磁性比较.宏观磁测量表明共沉淀法制备的样品在外磁场为1T时仍未饱和,磁化强度仅为46×10-3A·m2/g,在178K出现了超顺磁转变温度,且在测量温度范围内没有发现Verwey转变.     

Fe3O4@SiO2@TiO2复合纳米结构的尺寸与磁性调控

采用共沉淀法和溶剂热法制备了不同尺寸的Fe3O4纳米粒子,通过Stöber法和溶胶-凝胶法在Fe3O4磁核上包覆SiO2和TiO2壳层获得不同尺寸的Fe3O4@SiO2@TiO2复合纳米结构．采用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)和振动样品磁强计(VSM)等对其结构、形貌和磁性进行了研究．结果表明,大尺寸复合纳米粒子包覆均匀,分散性好,饱和磁化强度较大,有利于TiO2光催化剂的磁回收与再利用．     

复合磁性纳米NiFe2O4的制备及光谱特性

用微乳液化学剪裁方法制备了明胶包裹的复合纳米NiFe2 O4 。将明胶和亚铁盐以及镍盐制成凝胶 ,使该凝胶状反应物在微乳液的胶束中剪裁成微粒 ,再被还原 化合 成核长大。生成的微粒处于明胶蛋白分子的包裹之中。用XRD ,TEM ,EDS ,IR等测试表明 :微粒为明胶包裹球形纳米微粒。微球的平均粒径为 10～10 0nm ,单个微粒的粒径 3 3～ 4 6nm。每个复合微球中约有 3～ 2 2个NiFe2 O4 粒子。NiFe2 O4 复合微粉的比饱和磁化强度σs=36 31× 10 3 4π(A·m- 1 ·g- 1 ) ,矫顽力Hc=6 75 0A·m- 1 ,剩磁Br=4 39× 10 3 4π(A·m- 1 ·g- 1 )。     

用水热法合成掺杂Pr~(3+)的NiPr_xFe_(2-x)O_4纳米颗粒及其表征

采用水热法制备了掺杂Pr3+的NiPrx Fe2-x O4(x=0.0,0.01,0.025,0.05,0.075,0.1,0.15)纳米颗粒.实验结果表明制备的样品是立方体结构的纳米颗粒,当掺杂量为0x≤0.1时Pr3+能成功掺杂到NiFe2O4尖晶石晶格内,但掺杂量x0.1(x=0.15)时会出现杂峰.随着掺杂量从0增加到0.1,样品的平均晶粒尺寸从47nm减小到18nm,饱和磁化强度从55A·m2/kg单调减小至37A·m2/kg,矫顽力从4.7×103 A/m减小到3.4×103 A/m.饱和磁化强度减少的原因主要是由于室温下无磁性的Pr3+代替NiFe2O4中的Fe3+造成的.     

离子型钴铁氧体磁流体的稀土改性与机理研究

采用化学共沉淀法以柠檬酸三钠为表面改性剂制备了离子型稀土复合钴铁氧体磁流体.利用X衍射仪和透射电镜对磁粒子的组成、结构及粒径进行了分析.利用古埃磁天平和分光光度计研究了稀土离子改性对磁流体饱和磁化强度和磁感应的影响,实验结果表明:合成过程中添加稀土离子能明显降低磁性纳米粒子的粒径,制得的磁粒子均呈球形,钴铁氧体磁粒子的粒径为12～15nm,稀土钴铁氧体磁粒子的粒径为6～8nm.利用稀土改性的微观模型解释了粒径的降低.添加Dy3+能提高饱和磁化强度和磁感应,添加Y3+则能提高磁感应,却降低了饱和磁化强度.并从理论上对其改性机理进行了详细的分析.     

Keggin结构纳米硅钨酸铵的室温固相合成与物性

首次以H4SiW12 O40·2 2H2 O和 (NH4) 2 C2 O4·H2 O为原料 ,室温固相反应合成出 (NH4) 4 SiW12 O40 纳米微粒 ;用元素分析、FTIR确定产物的组成和结构 ;XRD、TEM和BET对产物的形貌、晶粒尺寸和比表面积进行了表征 ;TG DTA确定了产物的稳定温区 .结果表明 ,产物为纳米粒子 ,平均粒径为 6 0nm ,比表面积为 10 8.7m2 /g ,在 4 30℃以下具有良好的热稳定性 .在固相反应中 ,研磨和放热反应热效应能加快反应物扩散速率和生成物成核速率 ,使产物粒径减小 ;反应物含有结晶水和生成物H2 C2 O4·2H2 O ,对形成小粒径的 (NH4) 4 SiW12 O40 纳米粒子起关键作用 .     

NiFe_2O_4纳米粉末的制备及磁性研究

以硝酸铁、硝酸镍以及柠檬酸为原料,采用凝胶-热分解法制备了N iFe2O4纳米粉末。利用X射线衍射确定了粉体的相结构、比表面积和晶格常数,扫描电子显微镜(SEM)观察了颗粒的形貌,振动样品磁强计(VSM)测量样品的磁性能。结果表明:所制备的样品均为尖晶石结构,颗粒粒径为36nm~68nm,且颗粒的粒径随着热处理温度的升高而增大,样品的比饱和磁化强度最大可达54.63 emu/g。同时,文章也对反应的动力学原理进行了研究,得出N iFe2O4纳米颗粒形成的活化能为15.8kJ/mol。     

Controllable Synthesis and Magnetic Properties of Monodisperse Fe_3O_4 Nanoparticles

Magnetite(Fe_3O_4) nanoparticles with different sizes and shapes are synthesized by the thermal decomposition method.Two approaches,non-injection one-pot and hot-injection methods,are designed to investigate the growth mechanism in detail.It is found that the size and shape of nanoparticles are determined by adjusting the precursor concentration and duration time,which can be well explained by the mechanism based on the LaMer modei in our synthetic system.The monodisperse Fe_3O_4 nanoparticles have a mean diameter from 5nm to 16 nm,and shape evolution from spherical to triangular and cubic.The magnetic properties are size-dependent,and Fe_3O_4nanoparticles in small size about 5nm exhibit superparamagnetic properties at room temperature and maximum saturation magnetization approaches to 78 emu/g,whereas Fe_3O_4 nanoparticles develop ferromagnetic properties when the diameter increases to about 16 nm.     

Composites of nanotubular polyaniline containing Fe3O4 nanoparticles

Results of charge-transport and magnetic measurements of nanotubular polyaniline (PANI) composites containing Fe_3O_4 nanoparticles (～10nm) synthesized by a "template-free" method are reported. The T^{-1/2} resistivity has been observed, and dc magnetic susceptibility data are fitted to an equation χ=χ^*_P+C/T. With increasing weight ratio of Fe_3O_4, the electrical conductivity and temperature- independent susceptibility χ^*_P increase, and the Curie-type susceptibility is suppressed at low temperatures. Further discussions have been given. The PANI-H_3PO_4/Fe_3O_4 composite containing 27wt% of Fe_3O_4 nanoparticles is superparamagnetic, exhibiting very little hysteresis even at 5K.     

Radiation Losses in the Microwave X Band in Al-Cr Substituted Y-Type Hexaferrites

We present a study on radiation losses in the microwave X band in Al-Cr substituted Y-type hexaferrites,namely Ba_2 Mg_2 Al_(x/2)Cr_(x/2)Fe_(12-x)O_(22)(x= 0, 0.5 and 1.0). The study is performed by means of a vector network analyzer, Fourier transform infrared spectroscopy, a vibrating sample magnetometer and x-ray powder diffraction.Ba_2 Mg_2 Fe_(12)O_(22) hexaferrite shows radiation loss of-37.25 dB(99.999% loss) at frequency 9.81 GHz, which can be attributed to its high value of saturation magnetization, i.e., 22.08 emu/g. Moreover, we obtain that magnetic properties have strong influence on the radiation losses.     

Electrical and magnetic properties of polyaniline/Fe3O4 nanostructures

We report on electrical and magnetic properties of polyaniline (PANI) nanotubes (150 nm in diameter) and PANI/Fe₃O₄ nanowires (140 nm in diameter) containing Fe₃O₄ nanoparticles with a typical size of 12 nm. These systems were prepared by a template-free method. The conductivity of the nanostructures is 10⁻¹–10⁻² S/cm; and the temperature dependent resistivity follows a ln ρT^−1/2 law. The composites (6 and 20 wt% of Fe₃O₄) show a large negative magnetoresistance compared with that of pure PANI nanotubes and a considerably lower saturated magnetization (M_s=3.45 emu/g at 300 K and 4.21 emu/g at 4 K) compared with the values measured from bulk magnetite (M_s=84 emu/g) and pure Fe₃O₄ nanoparticles (M_s=65 emu/g). AC magnetic susceptibility was also measured. It is found that the peak position of the AC susceptibility of the nanocomposites shifts to a higher temperature (>245 K) compared with that of pure Fe₃O₄ nanoparticles (190–200 K). These results suggest that interactions between the polymer matrix and nanoparticles take place in these nanocomposites.     

Magnetic field aligned orderly arrangement of Fe_3O_4 nanoparticles in CS/PVA/Fe_3O_4 membranes

The CS/PVA/Fe_3O_4 nanocomposite membranes with chainlike arrangement of Fe_3O_4 nanoparticles are prepared by a magnetic-field-assisted solution casting method. The aim of this work is to investigate the relationship between the microstructure of the magnetic anisotropic CS/PVA/Fe_3O_4 membrane and the evolved macroscopic physicochemical property. With the same doping content, the relative crystallinity of CS/PVA/Fe_3O_4-M is lower than that of CS/PVA/Fe_3O_4.The Fourier transform infrared spectroscopy(FT-TR) measurements indicate that there is no chemical bonding between polymer molecule and Fe_3O_4 nanoparticle. The Fe_3O_4 nanoparticles in CS/PVA/Fe_3O_4 and CS/PVA/Fe_3O_4-M are wrapped by the chains of CS/PVA, which is also confirmed by scanning electron microscopy(SEM) and x-ray diffraction(XRD)analysis. The saturation magnetization value of CS/PVA/Fe_3O_4-M obviously increases compared with that of non-magnetic aligned membrane, meanwhile the transmittance decreases in the UV-visible region. The o-Ps lifetime distribution provides information about the free-volume nanoholes present in the amorphous region. It is suggested that the microstructure of CS/PVA/Fe_3O_4 membrane can be modified in its curing process under a magnetic field, which could affect the magnetic properties and the transmittance of nanocomposite membrane. In brief, a full understanding of the relationship between the microstructure and the macroscopic property of CS/PVA/Fe_3O_4 nanocomposite plays a vital role in exploring and designing the novel multifunctional materials.     

Synthesis and microwave absorption properties of graphene-oxide(GO)/polyaniline nanocomposite with Fe3O4 particles

In order to investigate the impedance matching properties of microwave absorbers,the ternary nanocomposites of GO/PANI/Fe₃O₄（GPF） are prepared via a two-step method,GO/PANI composites are synthesized by dilute polymerization in the presence of aniline monomer and GO,and GO/PANI/Fe₃O₄ is prepared via a co-precipitation method.The obtained nanocomposites are characterized by scanning electron microscopy（SEM）,X-ray diffraction（XRD）,and Fourier transform infrared spectroscopy（FTIR）,respectively.The microwave absorbability reveals enhanced microwave absorption properties compared with GO,PANI,and GO/PANI.The maximum reflection loss of GO/PANI/Fe₃O₄ is up to-27 dB at 14 GHz with its thickness being 2 mm,and its absorption bandwidths exceeding-10 dB are more than 11.2 GHz with its thickness values being in the range from 1.5 mm-4 mm.It provides that GO/PANI/Fe₃O₄ can be used as an attractive candidate for microwave absorbers.     

Enhanced hyperthermia performance in hard-soft magnetic mixed Zn0.5CoxFe2.5−xO4/SiO2 composite magnetic nanoparticles

High quality Zn0.5CoxFe2.5?xO4(x=0,0.05,0.1,0.15)serial magnetic nanoparticles with single cubic structures were prepared by the modified thermal decomposition method,and Zn0.5CoxFe2.5?xO4/SiO2 composite magnetic nanoparticles were prepared by surface modification of SiO2.The magnetic anisotropy of the sample increases with the increase of the doping amount of Co2+.When the doping amount is 0.1,the sample shows the transition from superparamagnetism to ferrimagnetism at room temperature.In the Zn0.5CoxFe2.5?xO4/SiO2 serial samples,the maximum value of specific loss power(SLP)with 1974 W/gmetal can also be found at doping amount of x=0.1.The composite nanoparticles are expected to be an excellent candidate for clinical magnetic hyperthermia.     

聚苯胺/钡铁氧体复合材料的制备及电磁性能

"采用原位掺杂聚合法,将聚苯胺对粒径在60~80 nm的M型钡铁氧体颗粒(BaFe12O19)进行包覆,得到了具有导电性和磁性的复合材料．通过X射线衍射、傅利叶变换红外光谱仪、扫描电镜和透射电镜等测试手段对材料的形貌和结构进行了表征．结果表明：PANI链段与BaFe12O19颗粒之间存在着作用力．使用振动磁强计和四探针法测定了复合材料的磁性能与电性能,其中50%复合材料的饱和磁化强度为22.2 emu/g,电导率为0.069 S/cm．"     

Novel Fe_3O_4@SiO_2@Ag@Ni trepang-like nanocomposites:High-efficiency and magnetic recyclable catalysts for organic dye degradation

A facile step-by-step approach is developed for synthesizing the high-efficiency and magnetic recyclable Fe_3O_4@SiO_2@Ag@Ni trepang-like nanocomposites.This method involves coating Fe_2O_3 nanorods with a uniform silica layer,reduction in 10%H_2/Ar atmosphere to transform the Fe_2O_3 into magnetic Fe_3O_4,and finally depositing Ag@Ni core-shell nanoparticles on the L-lysine modified surface of Fe_3O_4@SiO_2 nanorods.The fabricated nanocomposites are further characterized by x-ray diffraction,transmission electron microscopy,scanning electron microscope,Fourier transform infrared spectroscopy,and inductively coupled plasma mass spectroscopy.The Fe_3O_4@SiO_2@Ag@Ni trepang-like nanocomposites exhibit remarkably higher catalytic efficiency than monometallic Fe_3O_4@SiO_2@Ag nanocomposites toward the degradation of Rhodamine B(RhB) at room temperature,and maintain superior catalytic activity even after six cycles.In addition,these samples could be easily separated from the catalytic system by an external magnet and reused,which shows great potential applications in treating waste water.