稀土含量对快淬(Nd,Pr)x(FeCoZr)94-xB6粘结磁体磁性能的影响

采用工艺参数范围较宽的部分过快淬加晶化退火工艺，制备了快淬(Nd0．8Pr0.2)x(FeCoZr)94-xB6(x=12．0，10．5，10．0，9．0)粘结磁体，研究了稀土含量对磁体磁性能的影响规律。部分过快淬获得的由非晶和微晶共同组成的条屑，在实验优化的退火条件下晶化处理后，可获得最佳磁性能。稀土含量直接决定磁体的磁性能，随稀土含量的减少，磁体的剩磁Br增加，而内禀矫顽力Hti和最大磁能积(BH)m下降，10％是磁体磁性能发生较大变化的临界稀土含量。低于这一含量，合金中软磁相体积分数超出软磁相被完全耦合的临界值，Br增加缓慢，Hci和(BH)m迅速下降。这一实验结果与本文提出的完全耦合软磁相体积分数示意模型的计算结果相一致。     

高性能含镨快淬(Nd,Pr)12(FeCoZr)82B6粘结磁体的制备

采用过快淬加晶化退火处理的方法,研究了含有Pr的近正分快淬(Nd,Pr)12(FeCoZr)82B6粘结磁体制备工艺,粘结出的磁体磁性能为:Br=0.669T,Hci=811kA·m-1,Hcb=434kA·m-1,(BH)m=75kJ·m-3。合金快淬态的组成和显微结构、晶化退火温度、晶化退火时间直接影响磁体的磁性能,以24m·s-1速度快淬,并在655℃退火10min,可获得最佳磁性能。实验制备的粘结快淬(Nd,Pr)12(FeCeZr)82B6磁体(密度6 1g·cm-3)磁性能为:Br=0 669T,Hci=811kA·m-1,Hcb=434kA·m-1,(BH)m=75kJ·m-3     

Nd10.1Fe(83.7-x-y)CoxZryB6.2永磁材料结构和磁性能的研究

采用熔体快淬及晶化热处理工艺制备Nd10.1Fe(83.7-x-y)CoxZryB6.2纳米晶永磁材料. 在快淬速度为18 m·s-1时, 经710 ℃/4 min晶化处理后, Nd10.1Fe76Co5Zr2.7B6.2粘结磁体出现最佳磁性能, 分别为Br=0.67 T, JHc=754 kA·m-1, (BH)max=75.1 kJ·m-3. 粘结磁体的磁性能对于快淬速度非常敏感. 随着合金元素的添加, 出现最佳磁性能的快淬速度逐渐减少. 为了得到最佳磁性能, 除了选择合适的快淬速度外, 添加合适的合金元素变得非常重要.添加Zr元素抑制了亚稳相的析出以及细化了晶粒尺寸.比较不加Zr元素的Nd10.1Fe78.7Co5B6.2, 添加Zr元素晶化温度增加了9 ℃, 表明Zr元素也增加了快淬薄带的热稳定性.     

纳米晶复合Nd2Fe14B/α-Fe合金制备与磁性能的研究

采用熔体快淬及晶化处理工艺制备Nd11Fe71Co8V1.5Cr1B7.5纳米晶合金。经21m·s-1快淬及640℃ 4min晶化处理后,制成的粘结磁体的磁性能最佳,为:Br=0.64T,JHc=903.5kA·m-1,(BH)max=71kJ·m-3。添加Cr元素可提高内禀矫顽力,从而提高最大磁能积。     

铌和锆对(Nd,Pr)2Fe14B/α-Fe快淬合金晶化和磁性能的影响

研究了Nb和Zr添加对快淬纳米双相(Nd,Pr)2Fe14B/α-Fe合金晶化行为和磁性能的影响. 结果表明 (Nd0.4Pr0.6)8.5Fe85.5B6合金非晶晶化时, 在α-Fe相初始晶化后, 出现了(Nd,Pr)3Fe62B14亚稳相, 最终亚稳相分解形成(Nd,Pr)2Fe14B和α-Fe两相组织; (Nd0.4Pr0.6)8.5Fe84.5Nb0.5Zr0.5B6非晶晶化时, 同时析出α-Fe相和(Nd,Pr)2Fe14B相. 这说明添加Nb和Zr可避免亚稳相的形成并细化晶粒, 最大磁能积(BH)max从复合添加前的107.5上升到143.6 kJ·m-3. 而且, Nb和Zr原子在非晶晶化过程中可以部分取代Nd和Pr的晶位, 使稀土原子可以参与形成更多的硬磁相, 进一步提高了内禀矫顽力iHc. 合金(Nd0.4Pr0.6)8.5Fe84.5Zr0.5Nb0.5 B6经690 ℃退火10 min后磁性能最优, Br=1.10 T, iHc=534.2 kA·m-1, (BH)max=143.6 kJ·m-3.     

热处理对非晶态合金Nd_9(FeCoZrAl)_(85)B_6磁性能的影响

采用XRD等方法研究了单辊急冷法制备的低钕含量的快淬Nd9(FeCoZrAl) 85 B6 非晶态合金在不同热处理工艺下的相组成、晶粒尺寸大小及其磁性能变化规律。热处理工艺对Nd2 Fe1 4 B相和α Fe相析出、晶粒尺寸大小和合金的磁性能具有明显影响。当热处理温度较低时 ,Nd2 Fe1 4 B相析出不充分 ,并出现不均匀长大 ,其晶粒尺寸反而较大 ;当热处理温度过高时 ,Nd2 Fe1 4 B相虽然析出充分 ,但其晶粒尺寸也明显长大 ;只有当热处理温度适中 ( 685℃ /3 0min) ,既可保证Nd2 Fe1 4 B相析出充分 ,又不至于明显长大 ,才能使Nd2 Fe1 4 B相和α Fe相、Nd2 Fe1 4 B相和Nd2 Fe1 4 B相晶粒间的磁耦合效应达到最佳 ,从而增大剩磁 ,使该合金的磁性能也达到最佳 ,制得的粘结磁体性能 :剩磁Br=65 5mT ,内禀矫顽力jHc=64 4 3kA·m- 1 ,矫顽力bHc=3 79 0kA·m- 1 ,最大磁能积 (BH) m=65 68kJ·m- 3。     

添加镝的Nd-Fe-B纳米晶单相合金的微结构与磁性能研究

采用单辊快淬法制备了Nd12.3-xDyxFe79.7Zr0.8Nb0.8Cu0.4B6.0(x=0,0.5,1.5,2.5)合金纳米晶单相永磁薄带,研究了合金薄带晶化处理后,成分、组织结构与磁性能之间的关系.X射线衍射分析(XRD)表明,淬态合金主要由非晶相和Nd2Fe14B相组成,完全晶化后由Nd2Fe14B相和少量α-Fe组成.高分辨透射电镜(HRTEM)分析表明,经充分退火后,Nd2Fe14B晶体完整,晶粒间几乎没有边界相.随着Dy含量增加,晶粒尺寸细化,矫顽力大幅提高.x=0.5合金综合磁性能最佳,经过700℃晶化处理10min后,其磁性能为Jr=1.09 T,Hci=1048kA·m-1,(BH)max=169.5 kJ·m-3.     

Co含量对Pr10Fe74-xCo10+xC4B4 (x=0,2,4,6,8) 快淬条带的磁性能的影响

用快淬方法制备了Pr10Fe74-xCo10+xC4B4 (x=0,2,4,6,8) 条带,研究了成分和工艺对条带磁性能的影响.实验发现,当x=2,带速是20 m·s-1时,条带的磁性能最佳,其剩磁Jr=0.94 T,矫顽力μ0 iHc=0.96 T,最大磁能积 (BH)max=127.32 kJ·m-3.通过Henkel-plot分析,发现x=2,带速为20 m·s-1的样品中的晶间交换作用最强,因而能获得最佳的磁性能.     

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。     

双相纳米晶永磁体的研究

Nd8 .5Fe75Co5Cu1 Nb1 Zr3B6 .5合金熔体经 18m·s- 1 快淬 ,在 670℃ / 4min退火处理后 ,制备成的粘结磁体的最佳磁性能为 :Br=0 .68T(6 8kGs) ,JHc=62 0 .3kA·m- 1 (7 8kOe) ,(BH) max=74kJ·m- 3(9 3 3MGOe)。在低Nd合金中复合添加Zr和Cu ,提高了内禀矫顽力 ,改善了磁滞回线的矩形度 ,从而提高了最大磁能积。     

High-spin electronic states of lanthanide-arene complexes: Nd(benzene) and Nd(naphthalene)

Neodymium (Nd) complexes of benzene and naphthalene were synthesized in a laser-ablation supersonic molecular beam source. High-resolution electron spectra of these complexes were obtained using pulsed-field ionization zero electron kinetic energy (ZEKE) spectroscopy. Second-order M?ller-Plesset perturbation calculations were employed to aid spectral and electronic-state assignments. The adiabatic ionization energies were measured to be 38 081 (5) cm(-1) for Nd(benzene) and 37 815 (5) cm(-1) for Nd(naphthalene). For the Nd(benzene) complex, the observed frequencies of 831 and 286 cm(-1) were assigned to C-H out-of-plane bending and Nd(+)-C(6)H(6) stretching modes in the (6)A(1) ion state and 256 cm(-1) to the Nd-C(6)H(6) stretching mode in the (7)A(1) neutral state. To confirm these assignments, the ZEKE spectrum of the deuterated species was recorded, and the corresponding vibrational frequencies were measured to be 710 and 277 cm(-1) in the ion state and 236 cm(-1) in the neutral state. For the Nd(naphthalene) complex, the observed vibrational modes were C(10)H(8) bending (394 cm(-1)), Nd(+)-C(10)H(8) stretching (286 and 271 cm(-1)), Nd(+)-C(10)H(8) bending (80 cm(-1)), and C(10)H(8) twisting (105 cm(-1)) in the (6)A(') ion state and metal-ligand bending (60 cm(-1)) and ligand twisting (55 cm(-1)) in the (7)A(') neutral state. The formation of the ground state of the Nd(benzene) complex requires 4f → 5d and 6s → 5d electron excitation of the Nd atom, whereas the formation of the ground state of Nd(naphthalene) involves the 6s → 5d electron promotion.     

掺钕聚甲基丙烯酸甲酯的光学特性

Nd(DBM)3Phen-doped (DBM is dibenzoylmethane and Phen is phenanthroline) polymethyl methacrylate (PMMA) is prepared. Optical absorption, excitation and emission spectra were analyzed for Nd3+ in Nd(DBM)3Phen-doped PMMA. Using the Judd-Ofelt theory, the absorption spectrum was analyzed. The Judd-Ofelt(J-O) intensity parameters of Nd(DBM)3Phen-doped polymethyl methacrylate were calculated to be Ω2 = 20.97 × 10-20 cm2, Ω4 = 3.42 × 10-20 cm2, Ω6 = 2.90 × 10-20 cm2. The radiative lifetime (631 μs)of the excited 4F3/2 level is given. The stimulated emission cross-sections and the fluorescence branch ratios for the 4F3/2 →4 IJ/ transitions are also evaluated. Analysis reveals that Nd(DBM)3Phen-doped PMMA is promising for application in polymer optical fibers and planar waveguides.     

(H3O)Nd(SO4)2

The crystal structure of oxonium neodymium bis(sulfate), (H₃O)Nd(SO₄)₂, shows a two‐dimensional layered framework assembled from SO₄ tetrahedra and NdO₉ tricapped trigonal prisms. One independent sulfate group makes four S—O—Nd linkages, while the other makes five such connections to generate an unprecedented anhydrous anionic [Nd(SO₄)₂]⁻ layer. To achieve charge balance, H₃O⁺ cations are inserted between adjacent layers where they participate in hydrogen‐bonding interactions with the sulfate O atoms of adjacent layers.     

Studies on hypersensitive transitions of Nd(III) in Nd(III)-0-diketone-neutral ligand ternary compounds

In this paper, hypersensitive transitions of Nd( I) in Nd( I )-β-diketone-neutra] ligand ternary coordination compounds (where p-diketone = acetylacetone (AA), benzoylacetone (BA), dibenzoylmethane (DBM), 2-thenoyl trifluoroacetone (TTA); neutral ligand = pyridine (Py). cr.a′-dipyridyl (Dipy), phenanthroline (Phen) are studied and their intensities are given through dynamic coupling model. The results are in agreement with those observed and calculated using Judd-Ofelt equation. It may be seen that the dynamic coupling mechanism provides major contribution to the intensity of hypersensitive transition. On the other hand, in order to get the intensity of 4I_9/1→4G_5/2 transition, the absorption spectra in 560–610 nm have been decomposed into three peaks by nonlinear fitting with Lorentzian and Gaussian function and the “pure” intensities of hypersensitive transitions have been obtained, which are agreeable to those computed by Judd-Ofelt method and dynamic coupling model.     

热电离质谱法超高精度测定~(142)Nd/~(144)Nd同位素比

142Nd/144Nd比值的超高精度测定技术对于研究太阳系早期演化及月球-地球早期硅酸盐分异具有重要应用价值.本实验利用热电离质谱(TIMS)开展142Nd/144Nd比值的超高精度测试研究,并对比了动态多接收和静态多接收两种测量方式.结果表明,动态模式具有更高的准确度和精密度.讨论了影响测试精度的各种因素,在此基础上通过优化测试条件,对国际标准(Jndi-1)的142Nd/144Nd测试结果为1.1418348,外部精度优于5×10-6(2SD), 完全满足146Sm-142Nd体系研究的技术要求.     

Nd(O-i-C3H7)2Cl的直接合成法

Nd(O-i-C₃H₇)₂Cl可作为Ziegler-Natta催化剂中的主要成分用于共扼双烯的定向 聚合^[1],其常用合成方法^[1]需添加CH₃COCl: 我们在实验中发现,Nd(O-i-C₃H₇)₂Cl和异丙醇形成的络合物在苯-异丙醇混合溶液中并不沉淀析出,从而可用NdCl₃·3HO-i-C₃H₇,和NaO-i-C₃H₇,直接合成Nd(O-i-C₃H₇)₂Cl。     

Raman Spectra of Nd:La_3Ga_5SiO_(14) and Nd:La_3Ga_(5.5)Ta_(0.5)O_(14) Crystals

Single crystals of Nd:La_3Ga_5SiO_(14)(NLGS) and Nd:La_3Ga_(5.5)Ta_(0.5)O_(14)(NLGT) were grown by Czochralski method. Both crystals exhibit a langasite structure(space group D23(P321) with Z = 1), whose general formula is A_3BC_2D_3O_(14), where A, B, C and D represent the dodecahedral, octahedral and tetrahedral positions, respectively. The adding of low content of Nd does not change the crystal structure. Although they are isostructural, the distribution of atoms among the symmetric sites is different. While NLGT exhibits a perfect orderly structure, NLGS exhibits an intrinsically disordered structure due to the random distribution of Ga and Si atoms at the C3(2) symmetry sites. To understand what changes occur in the phonon distribution when Ta replaces Si, we recorded and analyzed room temperature polarized Raman spectra. We observe 8A1+18E modes for NLGS and 10A1+13E for NLGT crystals. When Si is substituted by Ta, we observe that the wavenumber of some modes related to vibrations involving Ga and O atoms decreases. This agrees with the fact that the Ga–O bonds are shorter in NLGS than in NLGT.     

Electrochemical study of the properties of Nd(III) and Nd(II) ions in molten LiCl-KCl-CsCl eutectic and individual CsCl

The electrochemical behavior of NdCl₃ solutions in eutectic LiCl-KCl-CsCl and individual CsCl melts was studied on an inert molybdenum electrode at temperatures in the range 573–943 K. Cyclic and differential pulse voltammetry and potentiometry at zero current and the electromotive forces method were used. The cathode reduction of Nd(III) ions to the metal was found to occur as a sequence of two stages. The formed Nd(II) ions were unstable above 798 K and underwent disproportionation 3Nd(II) ? 2Nd(III) + Nd_(m) in the salt melts. The conventional standard redox potential of the Nd(III)/Nd(II) pair in a eutectic LiCl-KCl-CsCl melt was measured over a wide temperature range. The main thermodynamic characteristics of the reaction NdCl_2(m) + 1/2Cl_2(g) ? NdCl_3(m) were determined.     

Thermochemistry of the Ternary Complex Nd（Et2dtc）3（phen）

Introduction A series of lanthanide sulfide complexes have beenlargely used for ceramics and thin film materials1 andthese complexes could be prepared from the precursorswhich are the compounds containing lanthanide-sulfurbonds.2-4 For instance, the compounds synthesized with[(alkyl)2dtc]-, phen?H2O and lanthanide salts were usedas the volatile precursors for preparing lanthanide sul-fide, its friction properties in lubricant was investigatedin literature 5 and the preparation and propertie…