Structural Stability and Magnetic Properties of the TbCu$_{7}$ -Type SmCo$_{x - 0.4}$Ti$_{0.4} (x = 5.0hbox{–}8.5)$ Alloys

We have studied the composition dependence, thermal stability, long-term stability at 500°C, and magnetic properties of the nanostructural TbCu₇-type (1:7) Sm-Co-Ti alloys. We prepared the SmCox-0.4Ti_0.4 alloys with a wide composition range from x = 5.0 to x = 8.5 by high-energy ball-milling, followed by annealing at 700-1100°C for 2 h. After annealing at 700°C, the powders with x = 7.0-8.5 showed a single 1:7 structure, while the powders with x = 5.0-6.5 presented the 1:7 plus CaCu₅-type (1:5) structure. At an annealing temperature higher than 800°C, a minor Th₂Zn₁₇-type (2:17) phase precipitated in the matrix of the 1:7 phase. Intrinsic coercivity iHc exhibits a maximum of 2.3 T at room temperature and 0.4 T at 500°C in the x = 7.0 samples annealed at 700°C. The temperature coefficient of iHc seems stable as the Sm/Co ratio changes from 1/6.5 to 1/7.5. The coercivity decreased with increasing annealing temperature Ta, from 2.3 T at Ta = 700°C to 1.3 T at Ta = 1100°C, which is mainly attributed to the grain growth from 35 nm for Ta = 700°C to 1 ?m for Ta = 1100°C. After holding at 500°C for up to 360 h, the microstructure and magnetic properties of the 1:7-type nanograin alloys remained almost unchanged, indicating a structurally and magnetically long-term stabilization at the potential high-temperature application environment.     

Structural and Magnetic Properties of MnFe$_1 - rm x$Co$_rm x$Ge Compounds

The structural and magnetic properties of MnFe_1-xCo_xGe compounds with x=0,0.1,0.2,0.3,0.4,0.5,0.6,0.7,0.8,0.85,0.9, and 1.0 were investigated by means of X-ray diffraction (XRD) and magnetization measurements. XRD shows that the MnFe_1-xCo_xGe compounds crystallize in the hexagonal Ni₂In-type crystal structure for xles0.8 and in the orthorhombic NiTiSi-type structure for x>0.8. The magnetization measurements show that the MnFe_1-xCo_xGe compounds exhibit a complex magnetic behavior. The Curie temperature increases with increasing of x. The saturation magnetization of the compounds with Ni₂In type structure increase with increasing of x and the saturation of the magnetization in the NiTiSi-type structure also increases with increasing x. We investigated the magnetocaloric effects in these compounds by means of magnetization measurements. The maximum magnetic-entropy change observed in these compounds reaches 9 J/kgK for x=0.8 in a field change from 0 to 5 T at around 289 K     

Formation and magnetostructural characterization of the novelternary compound Ce3Fe29-xMox

Formation and magnetostructural properties of the novel ternary ferromagnetic compound Ce₃Fe_29-xMo_x is reported. It was obtained in alloys with nominal compositions Ce₃ Fe_29-xMo_x, x=1.4, 1.5, and 1.6, prepared by arc melting and annealing during three weeks at 950°C. The crystal structure was well resolved as monoclinic with space group A2/m (No 12). Quantitative phase analysis, based on the processing of the X-ray diffraction patterns by the Rietveld method, was performed. Ce₃ Fe_29-xMo_x is the main phase (78-72 wt.%) with lattice parameters a=10.553(1) Å, b=8.511(1) Å, c=9.688(1) Å, and β=96.78(1)°. It coexists with Ce(Fe,Mo) ₁₂ as main spurious phase. Atomic positions and mean Fe-Fe interatomic distances are reported. Temperature-dependent magnetic susceptibility shows well-defined transitions at 7 and 115°C, which correspond to the 3:29 and 1:12 phases, respectively. Saturation magnetization at 4.2 K is 123 emu/g     

The (SmZr)Co$_3$Phase in Sm(CoFeCuZr)$_rm z$Magnets

Detailed microstructural characterization of magnets and homogenized as-cast alloys, which included X-ray diffraction Rietveld analysis, has indicated that the so-called platelet or lamellae phase is (SmZr)₁(CoFeCu)₃ with the PuNi₃ structure and lattice parameters a~0.5 nm and c~2.4 nm. The structural and magnetic properties of the (SmZr)Co₃ phase were investigated. The microstructure shows two phases differing in their Zr/Sm ratio. Magnetization curves for the samples (Sm_0.33Zr _0.67)Co₃, (Sm_0.33Zr_0.67)Co _2.97Fe_0.03, and (Sm_0.67Zr_0.33)Co₃ are consistent with the two-phase microstructure observed. Room temperature coercivity values of these samples are low (ap1 kOe.)     

Complex Permittivity and Permeability of Co$_2$U (Ba$_4$Co$_2$Fe$_36$O$_60$) Hexaferrite Bulk and Composite Thick Films at Radio and Microwave Frequencies

We measured dielectric, magnetic, and microwave properties of Co ₂U hexaferrite (Ba₄Co₂Fe₃₆O ₆₀) polycrystalline bulk and composite thick film samples, and studied the effect of annealing temperature on phase formation and microstructure. We synthesized the bulk samples from a precursor prepared by the citrate method. The values of dielectric constant at radio frequencies (50 Hz-1 MHz) of the bulk Co₂U12 sample sintered at 1200degC are much higher, and the resistivities are lower, compared to M-type barium hexaferrites. Coercivity is also low, having a value of 5 G for the Co₂U12 sample, whereas the saturation magnetization value is 59 emu/g, which is comparable to that of M-type hexaferrites. We also measured the complex permittivity and permeability for Co₂U12 samples at microwave frequencies and found the values high compared to M-type barium hexaferrite at these frequencies. Thick composite films were prepared from a ferrite-polymer mix, and all the above properties were studied for these films. We observed that these thick films have lower values of dielectric and magnetic parameters both at low and microwave frequencies. We measured microwave-absorbing properties for the ferrite-polymer sample (ferrite to polymer ratio 70/30) which showed a maximum reflection loss of -37.5 dB at 11.5 GHz for the 3.5-mm-thick sample     

Analytical electron microscopy of Sm(Co,Fe,Cu, Zr)9

Electron microscopic studies of as-cast Sm(Co,Fe,Cu,Zr)₉ magnets revealed a hexagonal phase of the type Sm₂(Co,Fe,Cu,Zr)₁₇ with crystal lattice parameters of a=0.84 nm and c=3.2 nm. After a solid solution treatment, only rhombohedral (3R) and hexagonal (2H) grains were found. After an additional annealing treatment at 800°C, grains with a microcellular precipitation structure similar to the one found in Sm(Co,Fe,Cu,Zr)_7.5 magnets occurred. In addition, in the as-cast and after-aged samples, other, partly unidentified Cu- or (Co,Fe)-enriched phases were detected     

Sintered Sm2(Co, Fe,Cu,Zr)17 magnets withlight rare earth substitutions

The effects of partial substitution of light rare earths for Sm in (Sm_1-xR_x)₂ (Co,Fe,Cu,Zr)₁₇ have been investigated where R=Ce, Pr, Nd, Pr_0.5Nd _0.5, Ce_0.2Pr_0.4Nd_0.4 and x=0-0.5. Experiments show that both remanence and maximum energy product are improved for x=0.1-0.2, depending upon compositions and heat treatments. For a composition Sm_0.8R_0.2(Co_0.633Fe_0.286 Cu_0.061Zr_0.020)_7.59 with R =Ce_0.2Pr_0.4Nd_0.4, the authors obtained B_r=11.57 kG, _MH_c =15.5 kOe, _BH_c=10.33 kOe, H_k=10.03 kOe, and (BH)_max=30 MGOe     

M位与A位双固溶MAX相的磁学性能研究

三元层状化合物MAX相兼具金属与陶瓷优良的力学性质,通常被认为是一类高安全结构材料。有研究显示,通过熔盐法可以将副族元素插入到MAX相A位层间,获得具有铁磁性能的V₂(Sn, A)C(A=Fe、Co、Ni和Mn)材料。因而,如何构建新的MAX相结构并实现其磁性调控备受关注。本研究通过MAX相M位和A位双固溶的方式设计了四种新型MAX相(V, Nb)₂(Sn, A)C(A=Fe、Co、Ni和Mn)。XRD、SEM、EDS结合TEM分析证实了上述新相的合成。超导量子磁强计(Superconducting quantum interference device magnetometer, SQUID)测试磁学性能发现, M位固溶后的MAX相的居里温度与其四方率(c/a)、元素组成有关。(V, Nb)₂(Sn, Fe)C、(V, Nb)₂(Sn, Ni)C、(V, Nb)₂(Sn, Mn)C相较于M位固溶Nb元素之前的V₂(Sn, A)C相,其矫顽力H_c...     

Piezoelectric properties in (K0.5Bi0.5)TiO 3-(Na0.5Bi0.5)TiO3-BaTiO 3 lead-free ceramics

Lead-free piezoelectric ceramics with compositions around the morphotropic phase boundary (MPB) x(Na_0.5Bi_0.5)TiO _3-y(K_0.5Bi_0.5)TiO₃-zBaTiO ₃ [x + y + z = 1; y:z = 2:1] were synthesized using conventional, solid-state processing. Dielectric maximum temperatures of 280degC and 262degC were found for tetragonal 0.79(Na_0.5Bi_0.5)TiO₃-0.14(K_0.5 Bi_0.5)TiO₃-0.07BaTiO$ d3 (BNBK79) and MPB composition 0.88(Na_0.5Bi_0.5)TiO₃-0.08(K _0.5Bi_0.5)TiO₃-0.04BaTiO$ d3 (BNBK88), with depolarization temperatures of 224degC and 162degC, respectively. Piezoelectric coefficients d₃₃ were found to be 135 pC/N and 170 pC/N for BNBK79 and BNBK88, and the piezoelectric d₃₁ was determined to be -37 pC/N and -51 pC/N, demonstrating strong anisotropy. Coercive field values were found to be 37 kV/cm and 29 kV/cm for BNBK79 and BNBK88, respectively. The remanent polarization of BNBK88 (~40 muC/cm²) was larger than that of BNBK79 (~29 muC/cm²). The piezoelectric, electromechanical, and high-field strain behaviors also were studied as a function of temperature and discussed     

Phase Transformation and Magnetostriction of (R-Pr)(Fe-T)_2 (R=Dy Tb; T=Co, Ni)

1. IntroductionMuch attention has been focused onmagnetostrictive materials RFe2, particularly,Tbo.zv~o.sDyo.vs~o.vFez (Terfenol-D), due to theirexcellellt magnetoelastic properties for the transducer deviceslll. Clark et al. firstly suggestedthat the pseudobinary compounds combined byTb, Dy and Fe could be constructed in an effortto reduce the anisotropy while maintaining largemagnetostrictionlZ]. Clark et al. also found in thecompensated system Tbl--.Pr.FeZ that (Tb, Pr)Fe3phase appea…     

Raman Studies of ${rm Ti}_{bm{ 1-x}} {rm Fe}_{bm x} {rm O}_{bm 2}$ Nanoparticles

Ti_1-xFe_xO₂ (x = 0.00-0.13) nanoparticle samples were prepared by hydrolysis method. We investigated the effects of Fe doping on the structural and magnetic properties of the Ti_1-xFe_xO₂ nanoparticle system. Scanning electron microscopy and X-ray diffraction measurements confirm that the particle size of the powder is in nanoscale, and that the magnetic Fe impurities substitute for the Ti sites in the anatase TiO₂ phase. All the samples with x > 0 were found to be super-paramagnetic at room temperature by magnetization measurements. Raman spectra also strongly support that the Fe atoms go into the Ti-site in theTiO₂ structure. For comparison, ceramic Ti_1-xFe_xO₂ samples were also prepared by usual ceramic method. Ferromagnetism was observed only in the ceramic Ti_1-xFe_xO₂ system. Additional Raman peak at around 610 cm^-1 is observed only in the ceramic samples. This may be related to the clusters created by mixture of various valence state of Fe, which probably would be the cause for ferromagnetism observed in the ceramic Ti_1-xFe_xO₂ system.     

Co0.525Fe0.475MnP化合物的室温磁热效应和磁电阻效应

采用多步骤固态烧结方法合成了具有单一Co₂P相的Co_0.525Fe_0.475MnP化合物,其反铁磁有序温度在室温附近。在升温过程中,这种化合物经历两个连续的磁转变：在285 K发生反铁磁到铁磁的一级相变,在375 K发生由铁磁到顺磁的二级相变。在0~5 T的外磁场中,两个相变点温度对应的最大磁熵变分别为1.1 J/(kg·K)(303 K)和-2.0 J/(kg·K)(383 K)。外磁场为零时,随着温度的降低电阻率曲线在铁磁到反铁磁转变温度附近出现极小值,是铁磁有序与反铁磁有序的竞争所致。在35 K再次出现的电阻率极小值,可归因于由Fe替代Co引起的自旋无序所导致的金属-绝缘体转变。在5 T磁场中磁电阻率的最大值对应温度为200 K时的-2.5%,在反铁磁温度以上磁电阻率迅速减小。这表明,这种化合物的磁电阻效应源于外磁场对反铁磁有序的影响。     

BaZrO3掺杂对(K0.49Na0.51)0.98Li0.02(Nb0.77Ta0.18Sb0.05)O3无铅压电陶瓷的结构与电性能的影响

采用固相反应法制备了(K_0.49Na_0.51)_0.98Li_0.02(Nb_0.77Ta_0.18Sb_0.05)O₃-xBaZrO₃ (NKNLST-xBZ, x = 0~0.020 mol)无铅压电陶瓷, 系统研究了BaZrO₃的掺杂量对陶瓷的压电、介电、机电和铁电性能的影响。结果表明: 随着BaZrO₃掺杂量x的增加, 陶瓷的晶体结构由正交相向四方相转变, 在x=0.005~0.008区间出现正交相与四方相两相共存的区域, 在此区域内陶瓷的晶粒变得细小且均匀, 介电损耗tanδ大幅降低, 压电常数d₃₃和平面机电耦合系数k_p增加。该体系陶瓷的介电常数ε T 33 /ε0则随着BaZrO₃的增加持续增加, 相变温度则向低温方向移动。当x=0.005时, 该组成陶瓷具有最佳的综合性能: 压电常数d33=372 pC/N, 平面机电耦合系数kp=47.2%, 介电损耗tanδ=3.1%, 以及较高的介电常数ε^T₃₃ /ε₀=1470和居里温度T_c=208℃。     

杂多酸离子液体负载氨基化Fe3O4磁性复合材料的制备及其超声辅助催化脱硫性能

以N-甲基咪唑、溴代正丁烷、磷钨酸为原料制备了1-丁基-3-甲基咪唑磷钨酸离子液体[BMIM]₃PW₁₂O₄₀,将其通过超声浸渍法负载于氨基化Fe₃O₄（Fe₃O₄-NH₂）,得到枣糕型结构的[BMIM]₃PW₁₂O₄₀/Fe₃O₄-NH₂磁性复合材料,通过FTIR、XRD、XPS、TEM、振动样品磁强计（VSM）、SEM等对其组成、形貌等进行表征。以[BMIM]₃PW₁₂O₄₀/Fe₃O₄-NH₂磁性复合材料为催化剂,以H₂O₂为氧化剂,催化氧化以二苯并噻吩为硫源的正辛烷模拟油样,通过单因素法分别考察了超声时间、H₂O₂用量、反应温度和催化剂用量等因素对脱硫效果的影响,并初步探讨了[BMIM]₃PW₁₂O₄₀/Fe₃O₄-NH₂磁性复合材料催化脱硫机制。结果表明:0.5 g/L[BMIM]₃PW₁₂O₄₀/Fe₃O₄-NH₂磁性复合材料超声辅助催化氧化浓度为500 mg/g模拟油样,在323 K下H₂O₂与二苯并噻吩的摩尔比n（O）:n（S）为8:1经超声10 min时,催化脱硫率达到最佳,为88.13%;重复使用5次后,[BMIM]₃PW₁₂O₄₀/Fe₃O₄-NH₂磁性复合材料对模拟油样的催化降解率仅下降了2.51%。说明该材料具有良好的催化脱硫性能,并可重复使用。催化机制初步研究表明,活性中心可能为杂多酸阴离子、Fe₃O₄-NH₂和离子液体分别起到载体和协同增容作用。      

Lattice matching of D023 and D022 phases in Al-6at.%(Ti,V,Zr) systems

Composite quaternary alloys with 21–22 vol.% of Al₃M (M = Ti,V,Zr) were made by vacuum arc melting. Two inlermetallic phases were found in alloys: one is V rich D0₂₂-Al₃(Ti,V,Zr) and the other is Zr rich D0₂₃-Al₃(Ti,V,Zr). Measured lattice constants of precipitate phases were strongly dependent on the composition of transition elements in precipitates and generally obeyed Vegard's rule. The lattice misfits between Al₃M phases and the matrix did not change much in alloys while the lattice misfit between D0₂₂ and D0₂₃ Al₃M phases was found to decrease with an increase in Ti content implying that the interface between both phases became more smooth, hard to distinguish and separate. A geometrical model was made for the lattice matching between two, D0₂₂ and D0₂₃ Al₃M phases. Titanium has been found to act as a retarding element to separation into D0₂₃ and D0₂₂ phases and the pre-existing phase may have been L₁₂ or D0₂₃ phase.     

Co掺杂GaFeO3陶瓷的结构、导电及磁性能研究(英文)

GaFeO₃因其磁电耦合效应成为目前极具潜质的多铁性材料之一。本工作采用固相烧结法制备了不同钴掺杂浓度的铁酸镓陶瓷,并研究了钴的掺杂浓度对铁酸镓陶瓷的相组成,微观结构形貌,漏电流及磁性的影响。XRD及Rietveld精修结果显示除了主相GaFeO₃,还存在第二相,且随着钴含量的增加,第二相含量逐渐增加,晶体的畸变程度增大;因为掺入二价阳离子Co²⁺并引入了第二相,样品的漏电性能和纯GaFeO₃陶瓷相比显著改善;当钴掺杂浓度为2at%时,样品的漏电流密度相较于GaFeO₃降低了7个数量级;掺入Co²⁺引入第二相且晶格畸变程度增加使得GaFeO₃的磁性增强。研究结果表明:铁酸镓中掺杂微量的钴可以改善磁性,并使漏电流大幅降低而磁转变温度无明显下降。     

Synthesis of Fe-substituted CoSb3-based skutterudite Co4–xFexSb12 by mechanical alloying-hot pressing-annealing

Mechanical alloying and preparation of Fesubstituted CoSb₃-based skutterudite Co_{4 x}Fe_xSb₁₂ (x"d1) were studied. All the compositions showed similar kinetics in mechanical alloying, where the skutterudite phase was kinetically more favorable than CoSb₂ phase initially. Then the latter became the strongest phase when milling time was increased. A single phase skutterudite structure could not be obtained via mechanical alloying. Hot pressing on powders milled for 10 hours yielded mostly skutterudite phase as well as minor residual Sb impurity, and single phase skutterudite compounds were finally obtained for Co_{4 x}Fe_xSb₁₂ (x"d0.65) after annealing at 650?C for 48 hours. The maximal solubility for Fe substitution seemed to be reached at x = 0.65.     

不同铁源制备磁性中空介孔硅铁复合微球及应用

采用一锅溶胶-凝胶法,以酚醛树脂为软模板、十六烷基三甲基溴化铵(CTAB)为制孔剂、四乙氧基硅烷(TEOS)为硅源,通过改变铁源制备了不同形貌的磁性中空介孔硅铁复合微球(Fe_xO_y/HMS),并考察了铁源在复合微球形成中的调控作用。利用 XRD、SEM、TEM以及振动样品磁强计(VSM)分别对其晶型结构、形貌和磁性进行了表征和分析。结果表明,乙酰丙酮铁(Fe(acac)₃)有助于复合微球壳层的形成,合成的复合微球更加光滑规整。对以Fe(acac)₃为铁源合成的Fe_xO_y/HMS复合微球磁性化后进行接枝聚丙烯腈(PAN),并经聚偕胺肟(PAO)化制得Fe_xO_y/HMS接枝聚偕胺肟(Fe_xO_y/HMS-g-PAO)复合材料,其比饱和磁化强度达8.6 emu/g,可用于水中Cr(Ⅵ)的吸附与快速分离。以浓度为100 mg/L的K₂Cr₂O₇溶液为目标溶液,pH = 2时平衡吸附量达123.75 mg/g。      

Tb掺杂双钙钛矿氧化物Pr2CoMnO6的磁热效应

采用高温固相反应法制备双钙钛矿氧化物Pr_(2-x)Tb_xCoMnO₆(x=0,0.05,0.1,0.15)系列陶瓷样品,研究了Tb的掺杂量对Pr₂CoMnO₆样品的居里温度、磁熵变以及磁相变的影响。结果表明:系列样品Pr_(2-x)Tb_xCoMnO₆(x=0,0.05,0.1,0.15)的空间点群为单斜晶系P2₁/n,具有良好的单相性;该组样品均有两个磁转变点(T_C1和T_C2);随着Tb掺杂量的增加T_C1和T_C2均降低下降;在测量温区内,随着温度的降低4个样品均先后经历顺磁态、顺磁-铁磁共存态;该组样品在7 T外加磁场中的最大磁熵变值ΔS_M分别为-1.862、-1.779、-1.768和-1.766 J/(kg·K)。掺杂Tb元素使最大磁熵变值变小,但是拓宽了半高宽温区。结合RCP值可以判断,Pr_1.9Tb_0.1CoMnO₆比其他三个样品更具有作为高温区磁制冷材料的潜能;根据对Arrott曲线、重标定曲线以及Loop曲线的分析,该组样品在此阶段经历了一级相变。     

海藻酸钙@Fe3O4/生物碳磁性复合材料的制备及其对Co (II)的吸附性能和机制

利用海藻酸钙（CA）包覆生物碳（BC）、Fe₃O₄制备了一种新型磁性微球（CA@Fe₃O₄/BC）,用以吸附水溶液中的Co（Ⅱ）。系统的研究了Co（NO₃）₂溶液浓度、pH和时间对吸附的影响。CA@Fe₃O₄/BC吸附Co（Ⅱ）等温热力学数据符合Langmuir模型,在pH=6的条件下对Co（Ⅱ）的最大吸附量为16.23 mg/g。研究显示,CA@Fe₃O₄/BC存在显著的协同效应,对Co（Ⅱ）具有更好的吸附性能。由于磁性颗粒的存在,CA@Fe₃O₄/BC吸附Co（Ⅱ）后可以用磁铁吸附快速分离。CA@Fe₃O₄/BC吸附Co（Ⅱ）动力学数据符合准二级动力学模型,研究表明,CA@Fe₃O₄/BC吸附Co（Ⅱ）的机制主要包括形成配合物及Ca（Ⅱ）与Co（Ⅱ）发生离子交换。