烧结Nd-Fe-B磁体的微观结构和冲击韧性研究

对烧结Nd₁₅Fe_72-xCo_yNb_xB₈(y=0, 5;x=0, 05, 10, 15, 20, 25)永磁体的微观结构和冲击韧性及二者间的关系进行了研究.结果表明，添加Nb能够改善Nd-Fe-B磁体的微观结构，提高磁体的冲击韧性.当无Co磁体中Nb的原子百分含量为15%时，其冲击韧性达到最大；对于添加了Co的磁体，其冲击韧性的     

金属有机物化学气相沉积法生长Ga2（1-x）In2xO3薄膜的结构及光电性能研究

采用金属有机物化学气相沉积（MOCVD）法在蓝宝石（0001）衬底上制备出了Ga_2（1-x）In_2xO₃（x=01—09）薄膜,研究了薄膜的结构、电学和光学特性以及退火处理对薄膜性质的影响.测量结果表明：当In组分x=02时,样品为单斜β-Ga₂O₃结构;x=05的样品,薄膜呈现非晶结构,退火处理后薄膜结构得到明显的改善 关键词： 金属有机物化学气相沉积 2（1-x）In_2xO₃薄膜')" href="#">Ga_2（1-x）In_2xO₃薄膜 蓝宝石衬底 退火     

Sr2Fe1－xCoxMoO6体系中Co的元素替代效应

在成功制备具有双钙钛矿结构Sr₂Fe_1-xCo_xMoO₆系列样品的基础上，对其结构、输运性质和磁性质进行了系统研究.结果发现，随着Co替代浓度x值的增加，样品的电阻率-温度关系由半金属行为转变为半导体行为，其室温电阻率从3.9×10^-5Ω·cm增大到6.0×10^-1Ω·cm；样品由亚铁磁体转变成反铁磁体，其磁相变温度T_N值也随之下降; Co对Fe的部分替代使其磁电阻效应受到抑制.基于对其电子结构的分析，其磁电阻效应的起源以及Co的元素替代效应也在文中进行了讨论. 关键词： 双钙钛矿结构 2FeMoO₆')" href="#">Sr₂FeMoO₆ 磁电阻     

Y掺杂SrTiO3晶体材料的电子结构计算

采用基于第一性原理的密度泛函理论平面波超软赝势法, 研究了Y掺杂SrTiO₃体系的空间结构和电子结构性质, 得到了优化后体系的结构参数, 掺杂形成能, 能带结构和电子态密度. 对比掺杂浓度为0125, 025, 033时,Sr_1-xY_xTiO₃和SrTi_1-xY_xO₃的掺杂形成能,发现Y替代Sr能形成更稳定的结构. 对Sr_1-xY_xTiO₃（x=0, 0125, 025, 033） 的结构进行了优化,结果表明Y替代Sr后, 随着掺杂浓度增大, 体系的晶格常数逐渐减小, 稳定性逐渐增强. 对不同掺杂浓度的Sr_1-xY_xTiO₃能带结构的计算结果表明：纯净的SrTiO₃是绝缘体, 价带顶在R点, 导带底在Γ点, 费米能级处于价带顶; 掺杂Y后, 费米能级进入到导带底中, 体系呈金属性;掺杂浓度越大,费米能级进入导带的位置越深,禁带宽度也近似变宽. 关键词： 3')" href="#">SrTiO₃ 电子结构 掺杂 VASP     

基态O和D原子的低能弹性碰撞及OD（X2Π）自由基的准确解析势与分子常数

利用CCSD（T）理论及相关一致五重基aug-cc-pV5Z构建了OD（X²Π）自由基的相互作用势, 计算了这个自由基的光谱常数D₀, D_e, R_e, ω_e, ω_eχe及B_e, 其值分别为44574,46225?eV,009702 nm, 2724923,453534和100096 cm^-1, 均与实验结果相符很好. 利用这一相互作用势, 在绝热近似下通过数值求解双原子分子核运动的径向薛定谔方程, 找到了J=0时OD（X²Π）自由基存在的全部23个振动态, 完整地求出了每一振动态的振动能级、振动经典转折点、惯性转动常数和离心畸变常数, 其值与实验结果相当一致. 在10×10^-11—10×10^-3a.u.的能量范围内研究了基态O和D原子沿OD（X²Π）势能曲线的弹性碰撞, 计算了这一碰撞的总截面和各分波截面, 分析了各分波截面对总截面的不同贡献. 结果表明: 总截面的形状主要由s分波截面决定, 尽管直到l = 12的其他分波截面均有形状共振存在, 但由于其强度较弱, 大都湮没在较强的s分波截面中. 关键词： 弹性碰撞 总截面 形状共振 光谱常数     

锰位铁掺杂La0.67Sr0.33FexMn1-xO3薄膜的光诱导效应

分别采用溶胶-凝胶法和脉冲激光沉积的方法制备了La_067Sr_033Fe_xMn_1-xO₃(x=0, 005, 010, 015)系列块材和薄膜,研究了Fe部分替代对La_067Sr_033Fe_xMn_1-xO₃薄膜 关键词： 光诱导 Fｅ掺杂 晶格效应     

B位等价掺杂SrBi4Ti4O15铁电材料的性能研究

采用了传统的固相烧结工艺,制备了不同Zr和Hf掺杂量的SrBi₄Ti_4-xZr_xO₁₅（x=000,003, 006,010,020）和SrBi₄Ti_4－xHf_xO₁₅（x=000,0005, 0015,0030,0060）的陶瓷 关键词： 4Ti_4-xZr_xO₁₅')" href="#">SrBi₄Ti_4-xZr_xO₁₅ 4Ti_4－xHf_xO₁₅')" href="#">SrBi₄Ti_4－xHf_xO₁₅ 铁电性能 介电性能     

Li(AlxCo1-x)O2晶体中Co3+电子态的变化及对结构演化的影响

研究了应用于锂二次电池正极的新型高能量密度存贮材料Li(AlxCo1-x)O2 (x=01—05)的磁性.发现Al3+的掺杂可导致Co3+中d电子自旋态发生变化，即有部分d电子进入高自旋态.伴随Co3+中电子状态的改变，材料结构演化也发生了相应变化，表现为c/a比增大明显减缓，较好地解释了材料结构对Vegard定律的正偏离.这对材料的微观结构与性能设计具有重要意义. 关键词： 锂电池材料 Li（AlxCo1-x）O2 磁性 自旋态 结构演化     

烧结Nd-Fe-B中的热力学影响

在烧结Nd-Fe-B中，各种相的形成，添加元素原子的替代、对磁体的微结构和性能的影响以 及大多数工艺与热力学都有密切联系.Al，Cu，Ga，Sn，Zn等与B均具有正的混合焓，在主相 中的浓度都很低，与富 Nd相反应改善磁体的微结构. Zi,Ti，Nb，W，Mo，V等与Nd有很大的 正的混合焓，与B具有很大的负的混合焓，能优化磁体的微结构和稀释磁体.参考热力学，系 统讨论了各种常用添加元素对烧结Nd-Fe-B的微结构、性能和制造工艺的影响. 关键词： Nd-Fe-B永磁体 混合焓 烧结     

Co掺杂对铁磁金属La0.8Sr0.2MnO3磁电阻影响机理

通过对La_0.8Sr_0.2Mn_1-yCo_yO₃(y≤02)饱和磁矩和输运的测量,研究了Co对La_0.8Sr_0.2MnO₃的磁电阻影响机制.结果表明,在La_0.8Sr_0.2Mn_1-yCo_yO₃（y≤02）中Co³⁺离子是低自旋态.由于Mn³⁺—O—Co³⁺—O—Mn³⁺类型的磁交换与Mn³⁺-Mn⁴⁺离子间双交换作用相比较弱,Curie温度T_C附近的磁电阻随着Co掺杂量的增加而降低.与此相反,由于Co²⁺离子与e_g巡游电子的反铁磁交换耦合作用,低温区间的磁电阻随着Co掺杂量的增加而升高. 关键词： 低自旋 磁电阻 磁交换作用     

Effect of Co on the thermal stability and impact toughness of sintered Nd–Fe–B magnets

The effect of Co on the thermal stability and impact toughness of sintered Nd–Fe–B magnets has been investigated. The results showed that the addition of Co decreased the intrinsic coercivity and the temperature coefficient of remanence (α), and increased the temperature coefficient of coercivity (β) for sintered Nd–Fe–B magnets. The impact toughness of sintered Nd–Fe–B magnets with the addition of Co first decreases, reaches a minimum, and then starts to increase. The possible reasons for increasing the temperature coefficients of coercivity (β) for sintered Nd–Fe–B magnets were analyzed, and the relations between the microstructure and impact toughness of sintered Nd–Fe–B magnets were studied.     

Effect of Tb on the intrinsic coercivity and impact toughness of sintered Nd–Dy–Fe–B magnets

The effect of Tb on the coercivity and impact toughness of sintered Nd–Dy–Fe–B magnets has been investigated. The results showed that the addition of Tb enhanced the intrinsic coercivity, reduced the remanence and improved the impact toughness of sintered magnets. The optimum impact toughness of sintered magnets was achieved when 1.0 at% Tb was incorporated. The possible reasons for increasing the intrinsic coercivity and improving impact toughness of sintered magnets were analyzed, and the relations between the microstructure and impact toughness of sintered magnets were studied.     

Nb含量对烧结NbFeB永磁体磁性能及显微结构的影响

关键词：     

Study of high-coercivity sintered NdFeB magnets

Magnetic powders for sintered NdFeB magnets have been prepared by using an advanced processing method including strip casting, hydrogen decrepitation, jet milling and rubber isotropic press. The effects of Dy, Ga and Co addition on the microstructure and magnetic properties of sintered magnets have been investigated. By adopting a suitable component ratio and adjusting proper technological parameters, we have prepared high-coercivity sintered NdFeB magnets with hard magnetic properties of _jH_c=25.6 kOe, B_r=13.2 kG and (BH)_max=39.9 MGOe. The temperature coefficient of coercivity of the magnets (between 20 and 150 °C) is –0.53%/°C. The magnetic properties at high temperature satisfy the needs of permanent magnet motors.     

烧结Nd-Fe-B磁体的磁性能一致性与其微观结构的关系

分析了微观结构和热处理工艺对矫顽力的影响,发现在矫顽力一定的情况下,磁体的微观结构越“差”,则保证不同批次磁体矫顽力变化不大于某一给定值所需的工艺条件就越严格;反之则越宽松.就同一炉产品而言,微观结构越好的磁体,其矫顽力受烧结(热处理)炉温度梯度的影响越小,其结果是该炉产品的一致性越高.反之,受温度梯度的影响越大,磁体的一致性也就越低.该研究结果说明:在条件许可的情况下,应首先考虑通过改善磁体的微观结构来提高磁性能一致性. 关键词： Nd-Fe-B永磁体 微观结构 内禀矫顽力 一致性     

烧结NdFeB断裂方式及其断面的微观结构

 经熔炼、制粉、成型、烧结和回火等工序制备了成分为Nd₃₃Fe_65.95B_1.05（质量分数）的烧结NdFeB磁体,将铸锭样品和烧结磁体样品折断,并采用扫描电子显微镜和金相显微镜对二者的断裂方式和断面的微观结构进行了对比分析。结果表明：烧结NdFeB铸锭的断裂方式为沿晶断裂,断面处有较多的层状富钕相,多边形的主相较为完整;烧结NdFeB磁体既有沿晶断裂也有穿晶断裂,但是以沿晶断裂为主。分析造成烧结NdFeB磁体断裂的原因为：（1）其微观结构中有大量的孔洞等缺陷,这是外部原因;（2）微观结构中占主要成分的主相的维氏硬度为6 235.94 N·mm^-2,富钕相的维氏硬度为5 947.42 N·mm^-2,二者有较大的差距,这是本征因素。针对磁体中孔洞和夹杂等缺陷存在而造成的断裂提出了相应的解决措施。     

Effect of γ-ray irradiation on the magnetic properties of NdFeB and Fe–Cr–Co permanent magnets

The effect of γ-ray irradiation on the magnetic properties of NdFeB and Fe–Cr–Co permanent magnets has been investigated. The magnetic flux loss of two kinds of magnets before and after irradiation was measured. Results show that the effect of γ-ray irradiation on the magnetic properties of sintered NdFeB is not so obvious as that on Fe–Cr–Co magnet. Irradiation-induced damage from γ-ray for the Fe–Cr–Co magnets was characterized for the first time. The decline of permanent magnetic properties of Fe–Cr–Co magnet induced by γ-ray irradiation is reversible except for the maximum energy product (BH)_max. The difference of coercivity mechanism between these two kinds of permanent magnets is responsible for the different dependence of magnetic properties loss induced by γ-ray irradiation.     

添加Nb在快淬NdFeB永磁体中的作用研究

系统研究了Nb元素的添加对快淬(Nd,Dy)_11.5Fe_82.4-nNb_nB_6.1(n=0,0.5,1,1.5,2)永磁体磁性能、温度特性及显微组织的影响. 结果表明：少量Nb元素的添加可以在不显著影响剩磁的情况下较大幅度提高磁体的内禀矫顽力，降低磁通不可逆损失. Nb在NdFeB磁体中的作用是使晶粒细小化、均匀化、规则化，提高交换耦合钉扎场H_p，减小材料内部的散磁场，显著降低磁通不可逆损失，改善NdFeB磁体在高温下的使用性能.     

Effects of powder flowability on the alignment degree and magnetic properties for NdFeB sintermagnets

The magnetic powders for sintered NdFeB magnets have been prepared by using the strip casting (SC), hydrogen decrepitation (HD) and jet milling (JM) techniques. The effects of powder flowability and addition of a lubricant on the alignment degree and the hard magnetic properties of sintered magnets have been studied. The results show that the main factor affecting powder flowability is the aggregation of magnetic particles for powders in a loose state, but it is the friction between the powder particles for powders that are in a compact state. The addition of a lubricant with suitable dose can slightly prevent the congregating of powders, obviously decrease the friction between the powder particles, improve the powder flowability, and increase the alignment degree, remanence and energy product density of sintered magnets. Mixing a suitable dose of lubricant and adopting rubber isostatic pressing (RIP) with a pulse magnetic field, we have succeeded in producing the sintered NdFeB magnet with high hard magnetic properties of B_r=14.57 KG, _jH_c=14.43 KOe, (BH)_max=51.3 MGOe.