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交换耦合

交换耦合的相关文献在1993年到2022年内共计234篇,主要集中在电工技术、物理学、金属学与金属工艺 等领域,其中期刊论文157篇、会议论文18篇、专利文献132029篇;相关期刊75种,包括材料导报、功能材料、稀土信息等; 相关会议14种,包括第十二届全国青年材料科学技术研讨会、中国稀土学会第一届青年学术会议、第四届全国纳米材料会议等;交换耦合的相关文献由553位作者贡献,包括李卫、都有为、夏爱林等。

交换耦合—发文量

期刊论文>

论文:157 占比:0.12%

会议论文>

论文:18 占比:0.01%

专利文献>

论文:132029 占比:99.87%

总计:132204篇

交换耦合—发文趋势图

交换耦合

-研究学者

  • 李卫
  • 都有为
  • 夏爱林
  • 晋传贵
  • 朱明刚
  • 顾本喜
  • 李华
  • 董建敏
  • 于广华
  • 小池文人
  • 期刊论文
  • 会议论文
  • 专利文献

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    • 张家榕; 陶姗; 葛洪良; 张朋越
    • 摘要: 采用铜模喷注法成功制备了尺寸为1×5×50 mm的长片状Nd7Fe61B22Mo4Y6合金.通过差式扫描量热分析、X射线衍射分析及磁性能测量系统研究了合金的热稳定性、相组成及磁性能.结果表明,合金的磁性能对于热处理条件极为敏感,铸态合金显示软磁性能,经不同温度热处理后,其磁性转变为硬磁特性.通过740°C等温退火10 min,合金表现出最佳磁学性能,其中剩磁0.51 T,矫顽力1289 kA/m,最大磁能积46.2 kJ/m3.Nd7Fe61B22Mo4Y6合金优良的磁性能可以归结为软磁相颗粒α-Fe、Fe3B和硬磁相颗粒Nd2Fe14B之间强烈的交换耦合作用.由于其尺寸大和磁性能良好的特点,Nd-Fe-B-Mo-Y系纳米复合永磁合金具有潜在的应用价值.
    • 徐钟麒; 刘畅; 罗维峰; 刘飞; 韩民
    • 摘要: 本文采用气相团簇束流沉积法制备了不同铁铬比的铁铬合金密集团簇点阵,研究了团簇点阵中复杂的多相结构和各种耦合效应.当合金中铬含量较大时,在团簇中能够观测到一种晶格失配的类四方结构,这种结构的出现导致了不同铁铬比的合金团簇中交换偏置效应的不同.随着铬的含量增加,合金团簇的交换偏置场减小,而团簇间的偶极相互作用增强.在合金团簇的铁磁-超顺磁转变温度以上,能明显观察到在类四方结构团簇中有更大的残存矫顽力与剩磁.在场冷条件下,对矫顽力和偏置场随温度变化的研究表明含有更多类四方结构的合金团簇有更好的热稳定性和更大的各向异性.
    • 谢海龙; 郑立允; 刘宏基
    • 摘要: 建立包含多晶微结构的微磁学模型,来研究软磁层的厚度、磁晶各向异性场、饱和磁化强度等本征磁性参数对CoPt-TiO2(6nm)/Co-TiO2(δ=1 ~4nm)交换耦合比特图形介质矫顽力的影响.发现当软磁层的厚度δ从1nm增加到4nm时,易磁化轴的矫顽力从8.2 kOe减小到5.8 kOe,归一化的剩余磁化强度Mr保持0.99基本没有变化.同时发现,当软磁层的磁晶各向异性场越小、饱和磁化强度越大,硬磁层的易磁化轴相对膜面法线方向倾斜的角度θ越大时,整个薄膜的矫顽力也越小.%In this paper,an accurate micromagnetic model is built for CoPt-TiO2 (6 rnm) / Co-TiO2(δ=1~ 4 nm) exchange coupled bit pattern media,based on the polycrystalline microstructure,to investigate the effect of the magnetic parameters such as the thickness,the anisotropy,the saturation magnetization of the soft layers on the coercivity of the bit pattern media.It is found that:the coercivity decreases from 8.2 kOe to 5.8 kOe when the thickness δ of the soft layer increases from 1 nm to 4 nm,whereas the normalized Mr remains 0.99.Meanwhile,the coercivity decreases when the anisotropy is lower,the saturation magnetization is larger in the soft layer and the angle θ is larger in the hard layer.
    • 陈兵; 蒋美琴; 肖恢芸; 潘晶; 刘新才
    • 摘要: The flakes of both Nd11.5Fe81.8B6.0Nb0.7and Nd67Cu33were prepared respectively at argon atmosphere within vacuum induction furnace.The mixed powder with 0,3%,6%,9% and 1 2% Nd67Cu33were hot-pressed and then die-upset.The microstructure evolution process of the die-upset magnets during the deformation and its effect on their coercivity have been discussed.The results show that when the deformation is increased from zero to 30%,the grain size ofα-Fe with neighbouring Nd-Cu particles decreases,the rich-rare earth phase ap-pears locally,and the rare-earth content of 2:14:1 partly compensates.The volume fraction of α-Fe in the magnets is reduced.And the exchange-spring effect is strengthened.So the coercive forces of the magnets are raised as the deformation increases.If it further does,the local rich-rare-earth phase disappears in the magnets with both 2:14:1 andα-Fe phase at last,and their grain sizes will enlarge.As soon as theα-Fe grain size is a-bove the critical exchange-spring one,its effect of the whole die-upset magnets will deteriorate.And the contri-bution of 2:14:1 with the larger grain size to the coercivity will fall.So the coercivity of the whole magnets will sharply cut down as the deformation further increases.At the deformation 70%,although the equivalent-average grain size is increased as the content of Nd67Cu33increasing,the coercivity of the die-upset magnets is still gone up.For the phenomena occur successively,α-Fe disappears,the rich-rare-earth gain boundary phase appears and its volume fraction increases,which enhances the magnetically decoupling.%分别真空感应快淬贫稀土钕铁硼合金Nd11.5Fe81.8B6.0Nb0.7与Nd67Cu33薄带,然后制备 Nd67Cu33含量0, 3%,6%,9%,12%(质量分数)的混粉热变形磁体,分析讨论了贫稀土钕铁硼合金与 Nd67Cu33混粉变形磁体中组织演变过程及其对磁体矫顽力的影响.研究结果表明,在热变形过程中当变形量由0增到30%时,混粉热变形磁体中Nd-Cu的扩散导致与之相邻区域的α-Fe晶粒尺寸减小、局部出现富稀土相、2:14:1相中稀土含量部分补偿性增加,整个磁体中α-Fe相体积分数减少、2:14:1相与软磁相α-Fe 交换耦合作用增强,混粉热变形磁体的矫顽力随变形量的增加而增大;当变形量进一步增加,在双相磁体中富稀土相消失,2:14:1相和α-Fe相晶粒尺寸增大,一旦α-Fe晶粒尺寸超过交换耦合的临界尺寸将导致双相交换耦合作用恶化,2:14:1相晶粒尺寸增大导致其对磁体矫顽力的贡献降低,整个混粉热变形磁体的矫顽力随变形量的增加而大幅度下降;当变形量达到70%时,混粉热压热变形磁体随Nd67Cu33添加量的增加尽管2:14:1等效平均晶粒尺寸增大但磁体的矫顽力不断提高,原因在于随Nd67Cu33的增加磁体分别出现α-Fe 消失、富稀土晶界相出现、且富稀土晶界相体积分数增大,富稀土晶界相的去磁耦合作用增强.
    • 胡晨宇; 泮敏翔; 张朋越; 葛洪良
    • 摘要: 通过高能球磨法制备了SmCo5/α-Fe纳米双相复合磁粉,研究了α-Fe含量对SmCo5/α-Fe纳米双相复合磁粉磁性能、微观结构及交换耦合作用的影响。XRD分析结果表明,α-Fe的复合没有改变SmCo5的晶体结构(仍为 CaCu5结构)。磁性能测试结果表明,随着α-Fe 含量的增加,SmCo5/α-Fe 纳米双相复合磁粉的矫顽力Hcj逐渐减小,剩磁Mr和最大磁能积(BH)max逐渐增大,当α-Fe含量为5wt%时,磁粉获得较优磁性能:Hcj=7.92kOe, Br=3.04kG,(BH)max=1.30MGOe。Henkel曲线表明,磁粉内部产生了强烈的交换耦合作用。%The SmCo5/α-Fe nanocomposite magnetic powders were prepared by high energy ball milling, and the influence ofα-Fe volume fraction on the magnetic properties, microstructure and exchange coupling were studied. The XRD results indicate that α-Fe complex does not change the crystal structure of SmCo5 (CaCu5 structure). Magnetic properties results show that with increasing α-Fe volume fraction, the coercivity (Hcj) of SmCo5/α-Fe nanocomposite magnetic powders decreases, the magnetization (Mr) and the maximum energy product (BH)max increase. The magnetic powders withα-Fe content of 5wt%have better magnetic properties:Hcj=7.92kOe, Mr=3.04kG, (BH)max=1.30MGOe. The Henkel-plot curve show a strong exchange coupling of the magnetic powders.
    • 刘静; 胡胜龙; 黄有林; 刘仲武
    • 摘要: NdδFe14B (δ=2.18~11) nanocrystalline ribbons were obtained by melt spining process, and their properties and mechanism of coercivity were studied. For NdδFe14B alloys prepared under optimal conditions, with increasing Nd content from 12.69 at% to 42.30 at%, the coercivity increases from 1021 kA/m to 1713 kA/m, the remanence decreases from 0.80 T to 0.38 T, and the values ofJs andJs/Js(Nd2Fe14B) also decrease gradually. The exchange coupling interaction may still exist in the Nd11Fe14B alloy forJr/Js=0.51>0.5. The relationship between coercivity (Hcj) and the particle spacing (R) was also investigated,and the results show thatHcjvalue is proportional toR by calculating and plot fitting.%通过直接甩带制备出不同富稀土含量的NdδFe14B(δ=2.18~11)纳米晶合金,并对其性能和矫顽力机理进行了研究。结果表明,在最佳条件下制备的NdδFe14B合金中,随着合金中Nd含量的增加,其矫顽力从1021kA/m提高到了1713kA/m,剩磁从0.80T减小到0.38T,饱和磁极化强度Js和Js/Js(Nd2Fe14B)逐渐减小,磁能积从104kJ/m3降低至29kJ/m3。其中,Nd2.82Fe14B合金的Jr/Js=0.52、Nd11Fe14B合金的Jr/Js=0.51,表明磁性颗粒间交换耦合作用仍然存在,但 Nd11Fe14B 的交换耦合作用相对较弱;两种薄带合金的矫顽力行为均具有钉扎机制特征。通过构建NdδFe14B合金矫顽力和硬磁性颗粒间相对距离之间的关系,发现其矫顽力和距离基本满足线性关系。
    • 李柱柏; 张雪峰; 李永峰; 刘艳丽; 赵倩
    • 摘要: 纳米复合磁体的磁能积能得到大幅度提高,前提是晶粒之间存在良好的交换耦合作用,而交换耦合作用与软、硬磁相之间的界面密切相关.对Nd2Fe14B、Sm-Co、FePt基纳米复合磁体界面交换耦合和反磁化的研究展开论述.在不同的条件下,界面结构的匹配性、界面原子扩散、晶间的非晶相、界面非磁性层、界面晶格弛豫等可能有利于改善界面的结构、增强交换耦合作用,进而对反磁化过程产生影响.反磁化的不可逆过程主要发生在硬磁相内,但与软、硬磁相界面特性密切相关.不可逆反磁化在一定程度上决定了磁体的矫顽力,它可通过改善界面结构进行调控.本文旨在对纳米复合磁体界面的作用深入理解并期望能对磁体磁性能的优化提供参考.
    • 薛允; 侯雪玲; 韩宁; 卢倩倩; 徐晖
    • 摘要: 利用X射线衍射(X-ray diffraction,XRD)分析仪、振动样品磁强计(vibrating sample magnetometer,VSM)和差示扫描量热仪(differential scanning calorimeter,DSC),研究了非晶Nd9.5Fe76Co5Ti3B6.5合金条带晶化过程中Nd2Fe14B/α-Fe析出相的相结构及其磁性能的变化.结果表明,在晶化过程中Nd2Fe14B相和α-Fe相分别在600,680°C退火时析出.随着退火温度的升高,α-Fe相的晶粒比Nd2Fe14B相长大更明显:当温度由690°C升高到700°C时,α-Fe相及Nd2Fe14B相的晶粒尺寸分别由22.4,32.8 nm长大到33.3,39.8 nm.在690°C退火时,硬磁相Nd2Fe14B和软磁相α-Fe之间具有较强的交换耦合作用,其晶粒尺寸分别为32.8,22.4 nm.此时的合金具有最佳的综合磁性能:剩磁强度Br=0.88 T,矫顽力Hi=523.76 kA/m,最大磁能积(BH)max=100.01 kJ/m3.
    • 李小英; 云国宏; 荣建红
    • 摘要: 利用能量极小原理研究了双层磁性薄膜系统中的铁磁共振特性,给出共振频率与线宽随外加磁场的变化关系.以及考虑应力各向异性、交换各向异性和单轴各向异性后,系统共振频率与线宽的变化情况.数值计算结果表明:外应力场和交换各向异性场对铁磁共振频率、频谱宽度以及磁化行为均有影响.
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