共查询到19条相似文献,搜索用时 203 毫秒
1.
将NiFe/PtMn双层膜生长在(Ni0.81Fe0.19)1-xCrx种子层材料上,通过改变种子层中Cr的原子含量,系统的研究了NiFe/PtMn双层膜中PtMn晶粒尺寸和织构对交换偏置的影响.对退火270℃,5h后的NiFe/PtMn双层膜磁性的研究表明,PtMn织构强弱对交换偏置场的影响不明显,而PtMn的晶粒尺寸是影响交换偏置场的主要因素,PtMn颗粒的相干长度在11.3nm左右时得到了较大的交换偏置场.
关键词:
NiFe/PtMn双层膜
交换偏置场 相似文献
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采用磁控溅射的方法制备了一组以(Ni0.81Fe0.19)1-xCrx作为缓冲层的NiFe/PtMn双层膜样品,研究了NiFe/PtMn双层膜的形成过程和热稳定性.实验表明,Cr成分的不同会引起NiFe/PtMn双层膜中PtMn层晶粒尺寸的不同,使NiFe/PtMn双层膜的交换偏置场与PtMn层厚度之间呈现不同的变化关系.热稳定性实验表明,PtMn晶粒尺寸较大的样品,出现交换偏置现象所需要的临界厚度较小,热稳定性好,这与Mauri的理论模型一致.
关键词:
NiFe/PtMn双层膜
交换偏置场
热稳定性 相似文献
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利用表面磁光克尔效应和铁磁共振对分子束外延生长的Fe/Fe50Mn50双层膜的交换偏置场和矫顽力进行了研究,实验结果表明,当反铁磁层厚度小于55nm时 ,不出现交换偏置,而当大于这一厚度时,出现交换偏置;大约在7nm时,达到极大值.随着 反铁磁层厚度的继续增大,偏置场和矫顽力随Fe50Mn50膜厚的增大 而下降.铁磁共振实验结果表明样品的磁性存在单向各向异性.并对上述结果进行了讨论.
关键词:
分子束外延
50Mn50')" href="#">Fe/Fe50Mn50
双层膜
交换偏置 相似文献
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采用快速液相烧结法制备BiFeO3和Bi0.95Dy0.05Fe1-xCoxO3 (x=0, 0.05, 0.1, 0.15)陶瓷样品. 实验结果表明: 所有样品的主衍射峰与纯相BiFeO3相符合且具有良好的晶体结构, 随着Co3+掺杂量的增大, Bi0.95Dy0.05Fe1-xCoxO3样品的主 衍射峰由双峰(104)与(110)逐渐重叠为单峰(110), 当掺杂量x>0.05时, 样品呈现正方晶系结构; SEM形貌分析可知: Dy3+, Co3+共掺杂使BiFeO3晶粒尺度由原来的3—5 μ减小到约1 μ. 室温下, BiFeO3样品表现出较弱的铁磁性, 随着Dy3+和Co3+掺杂, BiFeO3样品的铁磁性显著提高. 在外加磁场为30 kOe的作用下, Bi0.95Dy0.05Fe1-xCoxO3 (x=0.05, 0.1, 0.15)的Mr分别为0.43, 0.489, 0.973 emu/g; MS分别为0.77, 1.65, 3.08 emu/g. BiFeO3和Bi0.95Dy0.05Fe1-xCoxO3样品磁矩M随着温度T的升高而逐渐减小, Dy掺杂使BiFeO3样品的TN由644 K升高到648 K, 而TC基本没有变化. Dy和Co共掺杂导致BiFeO3样品磁相变温度TC由870 K降低到780 K, 其TC变化主要取决于Fe-O-Fe反铁磁超交换作用的强弱和磁结构的相对稳定性.
关键词:
铁磁电材料
磁滞回线
磁相变温度 相似文献
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用两带Ginzburg-Landau(GL)理论分析了Lu2Fe3Si5的表面临界磁场,当超导体的表面与任一主晶面重合,且外磁场平行于超导体的表面时,比值Hc3/Hc2(HC2是Lu2Fe3Si5的上临界磁场)强烈依赖于温度. 当超导体的表面是bc平面,且
关键词:
两带超导体
GL理论
2Fe3Si5')" href="#">Lu2Fe3Si5
表面临界磁场 相似文献
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用量子理论计算了Dy3Al5O12的晶场能谱、Zeeman劈裂能级和波函数. 在外磁场He为0<He<9 T, 温度为3<T<42 K 范围内, 计算了该晶体的磁矩、磁熵变, 计算结果与相关实验数据吻合较好. 该计算结果表明, Dy3Al5O12内磁性离子间的交换作用非常微弱, 可以忽略. 从理论上给出了绝热退磁过程中温度变化ΔT与T的关系, 并与Gd3Ga5O12晶体进行了比较, 发现不同外磁场下, Dy3Al5O12和Gd3Ga5O12的低温制冷性能在不同温区有差别. 在进行低温(T<10 K)制冷时, 若外磁场较低, 选择Dy3Al5O12作为磁制冷材料较好; 若外磁场较高, 选择Gd3Ga5O12作为磁制冷材料较好. 相似文献
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在一些磁性材料内, 磁性离子间交换作用和磁性离子的自旋涨落对材料磁性有影响. 本文根据磁比热实验值确定了晶场参数后, 利用包含自旋涨落的交换作用有效场Hm= n0 (1 + γ T + β eω T)M, 计算了PrNi2晶体晶场能级的Zeeman劈裂. 在温度为3.8 K ≤T≤ 30 K范围内, 计算了该晶体多晶磁矩随外磁场的变化, 以及外磁场H=5000 Oe时磁化率倒数随温度的变化, 计算结果和实验值符合较好. 当外磁场在0–50000 Oe时, 计算的该晶体的磁熵变与已有文献的理论结果相似. 计算结果说明, 提出的包含自旋涨落的交换作用有效场不仅适合亚铁磁性晶体, 而且也适合顺磁性晶体.
关键词:
2')" href="#">PrNi2
磁比热
交换作用有效场
磁矩
磁熵变 相似文献
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O. de Haas R. Schfer L. Schultz K. -U. Barholz R. Mattheis 《Journal of magnetism and magnetic materials》2003,260(3):380-385
The rotational magnetization process of an exchange coupled Ni81Fe19(10 nm)/Fe50Mn50(10 nm) bilayer was studied by Kerr microscopy. The domain processes in rotating magnetic fields near the exchange bias field Heb are very sensitive to local variations of coupling strength and direction. A characteristic domain splitting was found that shows a remarkably different behavior for weaker and stronger coupled areas. While the magnetization in weaker coupled areas follows the rotating field for H≈Heb, the stronger coupled areas switch back spring-like. As a result high-angle walls are formed between both areas causing rotational hysteresis. 相似文献
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This work describes multilayers of Co90Fe10 tF/Ru tRu/Co90Fe10 tF and Ni81Fe19 tF/Ru tRu/Ni81Fe19 tF (20 ÅtF200 Å) prepared at ambient temperature by ion beam deposition on Si/SiO2 3 kÅ substrates. The samples exhibited a maximum antiferromagnetic coupling with tRu=3.2 Å and M–H curves characterized by zero remanent magnetic moment and enhanced saturation field. Antiferromagnetic peaks were present with tRu17 and 30 Å. 相似文献
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Influence of temperature on thermal relaxation of exchange bias field in CoFe/Cu/CoFe/IrMn spin valve 下载免费PDF全文
《中国物理 B》2021,30(10):107501-107501
A multilayered spin valve film with a structure of Ta(5 nm)/Co_(75)Fe_(25)(5 nm)/Cu(2.5 nm)/Co_(75)Fe_(25)(5 nm)/Ir_(20)Mn_(80)(12 nm)/Ta(8 nm) is prepared by the high-vacuum direct current(DC) magnetron sputtering. The effect of temperature on the spin valve structure and the magnetic properties are studied by x-ray diffraction(XRD), atomic force microscopy(AFM), and vibrating sample magnetometry. The effect of temperature on the exchange bias field thermomagnetic properties of multilayered spin valve is studied by the residence time of samples in a reverse saturation field. The results show that as the temperature increases, the Ir Mn(111) texture weakens, surface/interface roughness increases, and the exchange bias field decreases. Below 200℃, the exchange bias field decreases with the residence time increasing, and at the beginning of the negative saturation field, the exchange bias field Hex decreases first quickly and then slowly gradually. When the temperature is greater than 200℃, the exchange bias field is unchanged with the residence time increasing. 相似文献
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D. W. Taylor V. Villas-Boas Q. Lu M. F. Rossignol F. P. Missell D. Givord S. Hirosawa 《Journal of magnetism and magnetic materials》1994,130(1-3):225-236
We studied the coercivity in magnets of composition R17Fe83−χBχ (R = Nd, Pr and χ = 8, 30), using measurements of the coercive field Hc, its angular dependence, and the magnetic viscosity coefficient Sv, for temperatures between 4.2 and 500 K. The results are discussed in relation to a model which does not specifically consider the detailed mechanisms involved in magnetization reversal, but which provides information about the magnetic properties in the activation volume v where magnetization reversal is initiated. It is concluded that the ordering temperature in v tends to be slightly smaller than in the bulk and that the room temperature anisotropy in v is not strongly reduced with respect to the bulk value. Finally, a direct evaluation of the dipolar interactions is in good agreement with results obtained from Hc(T). 相似文献
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Q. Y. Xu Z. M. Wang F. Shen Y. W. Du Z. Zhang 《Journal of magnetism and magnetic materials》2003,260(3):393-396
The anisotropic magnetoresistance (AMR) in permalloy Ni81Fe19 film deposited on a 1.2 nm Co33Cr67 buffer layer was significantly enhanced. The high-resolution electron microscopy was used to study the microstructure of Ni81Fe19 film with and without Co33Cr67 buffer layer. It was found that Co33Cr67 buffer layer can induce good (1 1 1) texture, while without Co33Cr67 buffer layer, Ni81Fe19 film show randomly oriented grain structure. The Δρ/ρ enhancement is attributed to the decrease in the resistivity ρ of the Ni81Fe19 film due to the formation of the large (1 1 1) textured grains in Ni81Fe19 film with Co33Cr67 buffer layer. However, the surface roughness of substrate may limit the (1 1 1) textured grain size and induce additional grain boundaries in Ni81Fe19 film with Co33Cr67 buffer layer, limit the enhancement of the AMR effect. 相似文献
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T. Saito Y. Matsumaru K. Shinagawa T. Tsushima 《Journal of magnetism and magnetic materials》1994,130(1-3):347-352
We have investigated critical lines in the H-T plane in a random anisotropy magnet (RAM) a-Dy16Fe84 with a small effective ratio of the anisotropy (D) to the exchange constant (J) by means of ac susceptibility (χ) in static fields H parallel and perpendicular to the ac field. We found that the transverse χ exhibits an anomaly along the irreversible line H(Tf) determined by previous magnetization measurements, while the longitudinal χ does so along a characteristic line H(Ti) in a lower temperature region. Above H(Tf) we also found an extra characteristic line H(Tc). The lines were almost independent of the measured frequency. Both the present results and previous magnetization results suggest that an equilibrium phase transition occurs, and the critical lines analogous to those in Heisenberg spin glasses are present in a weak RAM. 相似文献
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B. Dieny S.R. Teixeira B. Rodmacq C. Cowache S. Auffret O. Redon J. Pierre 《Journal of magnetism and magnetic materials》1994,130(1-3):197-215
We carried out a comprehensive study of structural, magnetic and electrotransport properties of as-deposited and annealed (Ni80Fe20)χAg(1−χ) heterogenous alloys prepared by sputtering. The NiFe atomic concentration was varied between 15% and 40%. These alloys consist of small magnetic particles (Ni80Fe20) embedded in a nonmagnetic matrix (Ag). The structures of these alloys were investigated by X-ray diffraction, scanning electron microscopy and high-resolution cross-section transmission electron microscopy. The magnetic measurements were made using SQUID magnetometry and ferromagnetic resonance. Magnetoresistance was measured with a conventional four-point probe between 1.5 K and room temperature in field range 0–6T. Three contributions to the magnetoresistance of these granular alloys have been clearly identified: the spin-valve (or giant) magnetoresistance as in multilayers, scattering on magnetic fluctuations (as in any ferromagnetic metal around its magnetic ordering temperature), and anisotropic magnetoresistance. These three contributions have their own dependences on the size of the magnetic particles, on the degree of intermixing between Ni80Fe20 and Ag, and on temperature. We discuss the different shapes and amplitudes of magnetoresistance versus Ni80Fe20 concentration or temperature and their evolution upon annealing in terms of the relative roles of these three contributions. The magnetoresistance in multilayers (current in-plane or perpendicular to the plane) and granular alloys are also compared. 相似文献
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In magnetic tunnel junctions a highly spin-polarizing layer is usually exchange biased by an antiferromagnetic layer, an artificial antiferromagnetic layer system or a combination of both, while the magnetically soft layer is free to rotate. The use of a single layer of a hard magnetic material is rarely investigated up to now. In this paper, we present the electric and magnetic properties of tunnel junctions with a hard magnetic Co83Cr17 layer. The soft magnetic electrode consists of either a single Co layer or a Co/Ni80Fe20 bilayer. The magnetic anisotropy and coercive field HC of the CoCr layer depend on its thickness and the kind of the bottom layer (Cu or Ta) and can vary from HC=50–700 Oe. It is found that a thin Co cap layer also influences the hysteretic behavior. Furthermore, only small changes after annealing up to 450°C promise a high thermal stability for the application in magnetic tunnel junctions. Measurements of the tunnel magnetoresistance on large area junctions, however, show a strong magnetic coupling of the hard and soft electrodes. 相似文献
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本文通过在新固相源中添加Ni2O3的方法, 采用顶部籽晶熔渗生长工艺(TSIG)制备出组分为(1-x) (Gd2O3+1.2BaCuO2)+x Ni2O3、直径为20 mm的单畴GdBCO 超导块材(其中x = 0, 0.02, 0.06, 0.10, 0.14, 0.18, 0.30, 0.50 wt%), 并研究了Ni2O3的掺杂量x对样品的表面生长形貌、微观结构、临界温度Tc、磁悬浮力以及俘获磁通密度的影响. 研究结果表明, 当Ni2O3的掺杂量x在0–0.50 wt%的范围内时, 均可制备出单畴性良好的样品, 且Ni2O3的掺杂对样品中Gd211粒子的分布和粒径没有明显的影响. 在Ni2O3的掺杂量x从0增加到0.50 wt%的过程中, 样品的临界温度Tc呈现下降的趋势, 从x=0时的92.5 K下降到x=0.50 wt%时的86.5 K, 这是由于Ni3 +替代GdBCO晶体中Cu2 +所致; 样品磁悬浮力和俘获磁通密度均呈现先增大后减小的变化规律, x=0.14 wt%时, 磁悬浮力达到最大值34.2 N, x=0.10 wt%时, 俘获磁通密度达到最大值0.354 T. 样品磁悬浮力和俘获磁通密度的变化规律与Ni2O3的掺杂量x有密切关系, 只有当掺杂量x合适时, Ni3+对Cu2 +的替代既不会造成Tc的明显下降, 但又能产生适量的Ni3 +/Cu2+ 晶格畸变, 从而达到提高样品磁通钉扎能力和超导性能的效果. 相似文献