Fe3O4／TiO2磁性催化剂的制备及在污水治理中的应用

以纳米Fe3O4为载体,以钛酸四丁酯为前躯体,用溶胶-凝胶法在Fe3O4表面包覆TiO2层,制备Fe3O4／TiO2光催化材料．透射电镜（TEM）、X射线衍射（XRD）、X射线光电子能谱（XPS）和红外光谱（IR）分析表明,TiO2在纳米Fe3O4颗粒表面形成很好的包覆层．用Fe3O4／TiO2光催化材料对工业上难处理...     

分子印迹聚吡咯/Fe3O4复合材料的制备及其在识别色氨酸光学异构体中的应用

首先利用共沉淀法合成了磁性材料Fe3O4,再以吡咯为单体,L-色氨酸为模板分子,采用化学聚合法使吡咯在Fe3O4表面发生原位聚合,同时通过分子间的作用力以及氢键作用将模板分子掺杂到Fe3O4表面的聚吡咯中,从而制备了分子印迹聚吡咯/Fe3O4复合材料,并且利用该材料的磁性质实现固液分离。在1 mol/L的NaOH溶液中,通过施加1 V的电位使聚吡咯发生过氧化从而使L-色氨酸模板分子脱掺杂。根据分子印迹的原理,该分子印迹的复合材料可用于识别L-色氨酸光学异构体。将扫描电镜、X射线衍射及电化学法用于该分子印迹复合材料的表征。将该材料填入到多孔陶瓷管,将L-和D-色氨酸溶液分别流过该多孔陶瓷管,流出液用高效液相色谱检测,发现该复合材料对于L-色氨酸的富集能力接近D-色氨酸的两倍,说明该复合材料具有作为手性识别色谱固定相的潜力。     

Fe3O4@SiO2@YF3:Eu3+磁-光双功能复合粒子的制备与性能

采用水热法合成了Fe3O4@SiO2@YF3:Eu3+磁-光双功能复合粒子,对其结构和性能进行了表征.XRD分析表明:Fe3O4表面包覆上了结晶良好的正交晶系的YF3.TEM照片表明:复合粒子为球形,构成核的Fe3O4颗粒的尺寸在200～350 nm之间,Fe3O4@SiO2@YF3:Eu3+核壳结构复合粒子的尺寸约为230～380 nm,与包覆前的Fe3O4相比较,包覆后,颗粒尺寸增大,并且YF3:Eu3+是以棒状结构连接在Fe3O4球型颗粒的表面.磁性和荧光光谱分析表明:该复合颗粒同时具有良好的发光性和磁性,使其在生物医学领域具有潜在的应用.     

纳米Fe3O4修饰电极制备及其催化应用

纳米Fe3O4修饰电极制备及其催化应用;纳米Fe3O4;修饰电极;多巴胺;测定;抗坏血酸(AA)     

Fe3O4纳米颗粒的表面改性

通过实验对Fe3O4纳米颗粒表面改性的最佳条件进行了摸索.并根据表面改性的包覆机理对不同酸度,温度和表面活性剂的用量对Fe3O4纳米颗粒的尺寸,磁性和稳定性的影响进行了理论上的分析.     

油分散性核壳Fe3O4@MnO纳米复合材料的合成及其对氧化环化反应的催化性能（英文）

采用两相种子介导法以锰油酸为前驱体制备了一种新型油溶性核壳结构Fe3O4@MnO纳米复合材料,直径约为15 nm。所制备的具有核壳结构的纳米复合材料是单分散且均匀的。该产物对2-羟基苯乙酮和1,2-二氨基苯的氧化环化反应表现出高且可循环的催化活性。与在环化反应中使用的其他报道的催化剂相比,所制备的Fe3O4@MnO纳米复合材料绿色、廉价且更适合于大规模工业应用。     

磁性纳米TiO2/Fe3O4光催化复合材料的制备及性能

采用溶胶-凝胶法，在磁性Fe3O4表面包覆TiO2，制备了一种新型纳米TiO2/Fe3O4光催化复合材料．XRD，TEM对材料形态结构及包覆情况的分析，显示TiO2包覆在Fe3O4表面，形成平均尺寸为35～50nm的复合结构；UV-vis吸收曲线表明，复合材料对光的吸收出现红移，吸收强度增大；对染料废水光催化降解的模拟研究表明，该复合材料对活性艳红染料的脱色率达100％，是一种便于回收、可重复使用的高效光催化剂．     

羟基磷灰石磁性复合材料用于水中砷(Ⅴ)的吸附

本文通过共沉淀法合成了不同质量比四氧化三铁(Fe3O4)/羟基磷灰石( Hydroxyapatite,HA)磁性复合材料作为新型吸附剂用于水中砷(Ⅴ)的吸附.研究了复合材料中Fe3O4质量百分比、吸附剂用量、pH值、吸附时间及温度对砷(Ⅴ)吸附性能的影响.结果表明,复合材料中Fe3O4质量百分比大于50％,复合材料用量...     

Fe3O4/C的制备与电化学性能研究

应用共沉淀法并以原位聚合苯胺包覆Fe3O4作碳源制备Fe3O4/C的复合材料.XRD、SEM、TEM等测试显示,样品中Fe3O4纳米颗粒(40～80 nm)均匀分散在无定形碳的内部.在50 mA.g-1电流密度下,经过30次循环充放电测试,该材料的容量仍保持在1000 mAh.g-1左右.     

Fe3O4@Gd2O3:Eu3+磁光双功能复合粒子的制备与表征

采用水热法合成了Fe3O4@Gd2O3:Eu3+核壳结构磁光双功能复合粒子,对其结构和性能进行了表征.XRD分析表明:700℃煅烧后Fe3O4表面包覆上了结晶良好的立方晶系的Gd2O3:Eu3+.TEM照片表明:所得的复合粒子具有明显的核壳结构和完美的球形,构成核的Fe3O4颗粒的尺寸在200～300 nm之间,Fe3...     

浅谈检验Fe~(2+)与Fe~(3+)的误区

空白试验证明,用浓度大于1mol/L的盐酸溶液做Fe~(3+)的提取液,或用过浓盐酸溶液酸化试液,盐酸中的Fe~(3+)都会给检验试液中的Fe~(3+)带来干扰;检验食品中的铁元素时,若铁是以Fe~(2+)形式存在,如果加入硝酸将其氧化为Fe~(3+),硝酸中Fe~(3+)会对检验试液中的Fe~(3+)带来干扰。     

The L Spectrum of Fe and Fe3O4

The intensities of the Fe L lines/bands l = L₃M₁, η = L₂M₁, α_1,2 = L₃M_4,5, β₁ = L₂M₄, and β_3,4 = L₁M_2,3 were measured for pure Fe and Fe₃O₄ using a TAP crystal as the dispersing element. The energy of the exciting electrons, E₀, was varied in the range 5 ≤ E₀ ≤ 25 keV. For pure Fe the following results were obtained. The net peak height ratio Ll/Lα remains relatively constant with varying E₀ at approximately 14%. The E₀ dependence of Lη is similar to that of Ll, although Lη is less intense than Ll by a factor of 7. Lβ₁/Lα decreases from 20% for E₀ = 5 keV to about 5% for 25 keV. Lβ_3,4 behaves like Lβ₁ but is weaker by a factor of 15. For Fe₃O₄ a much weaker intensity of Lα was observed which can be partially explained by its stronger absorption. Again, the E₀ dependence of Ll and Lη is similar with Ll/Lα = 19% and Lη/Lα = 4%. Lβ₁ and Lβ_3,4 show a comparable E₀ dependence. Lβ₁/Lα decreases from 50% for E₀ = 5 keV to 34% for 25 keV. Lβ_3,4 is weaker than Lβ₁ by a factor of about 25. The observed E₀ dependence of the different lines was used to estimate a set of mass absorption coefficients. Our value for Lα in Fe agrees well with other data which were deduced from variable E₀ measurements but differs considerably from data given by Heinrich and Henke.     

Influence of mechanical activation time,annealing, and Fe/O ratio on Fe3O4/Fe composites formation from Fe2O3 and Fe powders mixture

Commercially, iron (α-Fe) and hematite (α-Fe₂O₃) powders were used for the synthesis of composite powders of Fe₂O₃/Fe type by mechanical milling. Several ratios of Fe₂O₃/Fe were chosen for the composite synthesis; the atomic percent of oxygen in the starting mixtures ranged from 21 to 46 %. The Fe₂O₃/Fe composite samples with various Fe/O ratios were milled for different milling times. The milled composite samples were subjected to the heat treatments in argon up to 900 °C. During the heat treatment at temperatures that do not exceed 550 °C, Fe₃O₄/Fe composite particles are formed by the reaction between the Fe₂O₃ and Fe. Further increase of the heat treatment up to 700 °C leads to the reaction of the Fe₃O₄/Fe composite component phases, resulting thus in the formation of FeO/Fe composite. The heat treatment up to 900 °C of the Fe₂O₃/Fe leads to the formation of a composite of FeO/Fe₃O₄/Fe independent of the milling time and Fe₂O₃/Fe ratios. The onset temperatures of the Fe₃O₄ and FeO formations decrease upon increasing the milling time. Another important aspect is that, in the case of the same milling time but with a large amount of iron into the composite powder the formations temperatures of Fe₃O₄ and FeO are also decreasing. The influence of the mechanical activation time, heat treatment temperature, and Fe/O ratio on the formation of the (Fe₃O₄, FeO)/Fe composite from Fe₂O₃+Fe precursor mixtures was studied by differential scanning calorimetry and X-ray diffraction techniques.     

Structure and properties of iron oxide clusters: From Fe6 to Fe6O20 and from Fe7 to Fe7O24

Geometrical and electronic structures of the neutral and singly negatively charged Fe₆O_n and Fe₇O_m clusters in the range of 1 ≤ n ≤ 20 and 1 ≤ m ≤ 24, respectively, are computed using density functional theory with the generalized gradient approximation. The largest clusters in the two series, Fe₆O₂₀ and Fe₇O₂₄, can be described as Fe(FeO₄)₅ and Fe(FeO₄)₆ or alternatively as [FeO₅](FeO₃)₅ and [FeO₆](FeO₃)₆, respectively. The Fe₆O₂₀ and Fe₇O₂₄ clusters possess adiabatic electron affinities (EA_ad) of 5.64 eV and 5.80 eV and can be attributed to the class of hyperhalogens since FeO₄ is an unique closed‐shell superhalogen with the EA_ad of 3.9 eV. The spin character of the lowest total energy states in both series changes from ferromagnetic to ferrimagnetic or antiferromagnetic when the first Fe? O? Fe bridge is formed. Oxidation decreases substantially the polarizability per atom of the initial bare clusters; namely, from 5.98 ų of Fe₆ to 2.47 ų of Fe₆O₂₀ and from 5.67 ų of Fe₇ to 2.38 ų of Fe₇O₂₄. The results of our computations pertaining to the binding energies of O, Fe, O₂, and FeO in the Fe₇O_m series provide an explanation for the experimentally observed abundance of the iron oxide nanoparticles with stoichiometric compositions. © 2016 Wiley Periodicals, Inc.     

Synthesis and characterisation of Fe6 and Fe12 clusters using bicine

Reaction of bicine {BicH₃, N,N-bis(2-hydroxyethyl)glycine} with an Fe(III) oxo-centered pivalate triangle in MeCN in the presence of Et₂NH yields [Et₂NH₂]₂[Fe₆O₂(OH)₂(Bic)₂(O₂CCMe₃)₈], which possesses an S = 5 ground state.Changing the base to NaOMe produces [Fe₁₂O₄(Bic)₄(HBic)₄(O₂CCMe₃)₈], which contains two Fe₆ units bridged by the carboxylate arms from the bicine ligands. The complex displays strong antiferromagnetic coupling leading to an S = 0 ground state.     

Oxygen on Fe(100) and Fe(110)

Investigations of the electronic and magnetic properties of oxygen adsorbed on magnetized iron films have been carried out by means of angle and spin resolving photoelectron spectroscopy. Iron, epitaxially grown on W(100) and W(110) crystals, served as the ferromagnetic substrate. Exchange splittings of the O 2p_x derived level have been detected, demonstrating a magnetic coupling between the chemisorbate and the iron layer. Variations of the exchange splitting have occurred as a function of the oxygen coverage, photon energy, and emission angle. High oxygen exposures have lead to a FeO overlayer at the surface.     

Oxygen on Fe(100) and Fe(110)

Investigations of the electronic and magnetic properties of oxygen adsorbed on magnetized iron films have been carried out by means of angle and spin resolving photoelectron spectroscopy. Iron, epitaxially grown on W(100) and W(110) crystals, served as the ferromagnetic substrate. Exchange splittings of the O 2p_x derived level have been detected, demonstrating a magnetic coupling between the chemisorbate and the iron layer. Variations of the exchange splitting have occurred as a function of the oxygen coverage, photon energy, and emission angle. High oxygen exposures have lead to a FeO overlayer at the surface.     

Methanolysis and phenolysis routes to Fe6, Fe8, and Fe1) complexes and their magnetic properties: a new type of Fe8 ferric wheel

Alcoholysis of preformed tetranuclear and hexanuclear iron(III) clusters has been employed for the synthesis of four higher-nuclearity clusters. Treatment of [Fe(4)O(2)(O(2)CMe)(7)(bpy)(2)](ClO(4)) with phenol affords the hexanuclear cluster [Fe(6)O(3)(O(2)CMe)(9)(OPh)(2)(bpy)(2)](ClO(4)) (1). Reaction of [Fe(6)O(2)(OH)(2)(O(2)CR)(10)(hep)(2)] (R = Bu(t) or Ph) with PhOH affords the new "ferric wheel" complexes [Fe(8)(OH)(4)(OPh)(8)(O(2)CR)(12)] [R = Bu(t) (2) or Ph (3)]. Complexes 2 and 3 exhibit the same structure, which is an unprecedented type for Fe(III). In contrast, treatment of [Fe(6)O(2)(OH)(2)(O(2)CBu(t))(10)(hep)(2)] with MeOH leads to the formation of [Fe(10)(OMe)(20)(O(2)CBu(t))(10)] (4), which exhibits the more common type of ferric wheel seen in analogous complexes with other carboxylate groups. Solid-state variable-temperature magnetic susceptibility measurements indicate spin-singlet ground states for complexes 2 and 4. The recently developed semiempirical method ZILSH was used to estimate the pairwise exchange parameters (J(AB)) and the average spin couplings S(A)[empty set].S(B)[empty set] between the Fe(III) centers, providing a clear depiction of the overall magnetic behavior of the molecules. All exchange interactions between adjacent Fe(III) atoms are antiferromagnetic.     

Syntheses,structures and magnetic properties of Fe6 and Fe12 ferric wheels

Starting from the same Fe3O(RCO2)6 complex and using a similar synthesis strategy, the Fe6 and Fe12 wheels were obtained by utilizing two designed ligands, 2-amino-2-methyl-1,3-propanediol(L1) and 1,3-propanediol(L2), respectively. A biological buffer reagent, Bis-Tris(2-[bis-(2-hydroxyethyl)amino]-2-(hydroxymethyl)propane-1,3-diol) was first introduced in the synthesis of the Fe12 wheel, playing a vital role in adjusting the acidity of reaction environment. Magnetic studies on both Fe6 and Fe12 wheels revealed strong antiferromagnetic coupling between the spins on FeIII ions.