共查询到18条相似文献,搜索用时 218 毫秒
1.
研究了结构为 (FM/SiO2)3/Ag/(SiO2/FM)3 多层膜的巨磁阻抗(GMI)效应(这里的F M≡FeCuCrVSiB).多层膜采用射频溅射法沉积在单晶Si衬底上,沉积过程中,沿膜面长方 向施加约72kA/m的磁场,然后在不同的温度下对样品进行了退火处理.结果表明,该多层膜 样品即使在沉积态便具有相当好的软磁性能和GMI效应,在7MHz的频率下,最大纵向和横向 巨磁阻抗比分别为45%和44%.在230℃下经90min退火处理后的样品具有最佳的GMI效应,在85MHz的频率下,最大纵向和横向巨磁阻抗比分别达到251%和277%.与磁性层总厚度相同的FeCuCrVSiB/Ag/FeCuCrVSiB三层膜相比较,在这种多层结构中出现的GMI效应更强.
关键词:
多层膜
巨磁阻抗效应
趋肤效应
有效磁导率 相似文献
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将600℃退火后的超磁致伸缩材料(Tb0.27Dy0.73)0.3Fe0.7薄膜作为Ni80.2Fe14.1Si0.2Mn0.4Mo5.1三明治膜的基底,制备出四层膜.结果表明:附加的磁致伸缩并没有减小材料的巨磁阻抗(GMI)效应,而由于磁场下磁致伸缩材料的应力效应影响了三明治膜中的各向异性场,使三明治膜的GMI效应增大了4倍.再将制备态的四层膜在280℃下真空退火,退火态四层膜也增大了三明治膜的GMI效应,但可能由于磁致伸缩向磁性层中的扩散,其GMI效应相对于制备态四层膜则有所降低.
关键词:
巨磁阻抗(GMI)效应
三明治膜
TbDyFe薄膜
各向异性场 相似文献
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用射频溅射法制备了Fe73.5Cu1Nb3Si13.5B9单层膜和 Cu或Ag作为中间层的三明治膜.溅态膜为非晶态结构.磁畴观察结果表明,单层膜在380℃退火后,呈现均匀磁化的纳米晶结构,该样品软磁特性最佳,其巨磁阻抗效应最大,在13MHz,最大磁阻抗比纵向为18%,横向为14%.溅态三明治膜具有较大的巨磁阻抗效应,在13MHz,Cu夹层三明治膜的最大磁阻抗比纵向为32%,横向为11%,Ag夹层三明治膜的最大磁阻抗比纵向为47%,横向为57%.Cu夹层三明治膜经250℃退火后,在低频下表现为巨磁电感效应,在100kHz,最大磁电感比为1733%.
关键词: 相似文献
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采用电子束蒸发法制备的81NiFe/Cr多层膜具有单向各向异性,磁滞回线非轴对称,相当存在1Oe数量级的交换偏场。磁电阻回线的上升和下降两枝差别明显,其中以横向磁电阻回线最为显著。有的试样上升枝与下降枝相应的最大横向磁电阻率之差已高达0.78%,其最大各向异性磁电阻率(Rmax-Rmin)/R为4.72%,甚高于Miyazaki等[1]的优质82NiFe合金单层膜的报道值3%。可以认为这类多层膜的磁电阻效应除主要来源于自旋-轨道耦合机制外,
关键词: 相似文献
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高硬度的含氧化物纳米多层膜在工具涂层上具有重要的应用价值.研究了TiN/SiO22纳米多 层膜的晶体生长特征和超硬效应.一系列具有不同SiO22和TiN调制层厚的纳米多 层膜采用多 靶磁控溅射法制备;采用x射线衍射、x射线能量色散谱、高分辨电子显微镜和微力学探针表 征了多层膜的微结构和力学性能.结果表明,虽然以单层膜形式存在的TiN和SiO22分别形成 纳米晶和非晶结构,它们组成多层膜时会因晶体生长的互促效应而呈现共格外延生长的结构 特
关键词:
2纳米多层膜')" href="#">TiN/SiO22纳米多层膜
外延生长
非晶晶化
超硬效应 相似文献
7.
利用磁控溅射方法在100℃的MgO单晶基片上制备了[FePt/Au]10多层膜,并研究了采用FePt/Au多层膜结构对FePt薄膜的有序化温度、矫顽力(HC)、垂直磁各向异性、晶粒尺寸以及颗粒间磁交换耦合作用的影响.磁性测试结果表明:FePt/Au多层膜在退火后具有较高的HC、良好的垂直磁各向异性、较小的晶粒尺寸且无磁交换耦合作用.截面高分辨电镜分析表明:Au可以缓解MgO和FePt之间较大的晶格错配,从而促进薄
关键词:
0-FePt薄膜')" href="#">L10-FePt薄膜
有序化温度
垂直磁各向异性
磁交换耦合作用 相似文献
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利用脉冲激光沉积方法在Si(100)上制备了Cox-C1-x颗粒膜,并研 究了其正磁电阻 效应.实验结果表明,样品在室温下的正磁电阻效应要远远高于低温下的正磁电阻效应;Co 0.02-C0.98样品具有最大的室温正磁电阻效应,在外加磁场B=1T时 ,其磁电阻 率MR=22%;随着Co含量的增加,Cox-C1-x颗粒膜的正磁电阻效应呈 减小趋势.样品 的MR-B的曲线与传统的多
关键词:
正磁电阻效应
x-C1-x颗粒膜')" href="#">Cox-C1-x颗粒膜
脉冲激光沉积 相似文献
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用射频溅射法制备了FeZrBCu软磁合金薄膜.研究了不同溅射功率对FeZrBCu薄膜软磁特性和巨磁阻抗效应的影响.用电子探针显微镜测量发现,当溅射功率为240W时,薄膜样品中Fe的原子含量为8732%,Cu的原子含量为29%.这种样品的矫顽力最小,为68A/m,饱和磁化强度约为111×1055A/m,软磁性能最佳,巨磁阻抗效应最大,溅态膜在 13MHz最大巨磁阻抗比纵向为17%,横向为11%.重点分析了阻抗的电阻、电感分量及横向有 效磁导率随频率的变化,得到在低频下主要是磁电感
关键词:
铁基合金
薄膜
巨磁阻抗效应 相似文献
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采用层间胶合方法制备了淬态非晶FeSiB/Cu/FeSiB三明治薄带,研究了同尺寸单层薄带和三明治薄带的巨磁阻抗(giant magneto-impedance, GMI)随外磁场与带轴夹角β的变化特性.结果表明,FeSiB单层薄带在7.0 MHz最佳响应频率下,GMI仅约30%,外磁场与带轴夹角对单层薄带GMI几乎没有影响;三明治薄带的GMI效应则十分显著,在0.6 MHz最佳响应频率下,纵、横向GMI比分别达到272%和464%, GMI随β的增大而增强;所有β角的三明治薄带GMI曲线都出现各向异性峰,各向异性峰随β的增大而展宽.根据磁畴转动模型推导了薄带横向磁导率与各向异性场及β之间的函数关系式.结果显示,三明治薄带GMI随夹角β变化的特性与理论推算的横向磁导率变化有较好的一致性,而单层薄带则不然.该磁畴转动模型能定性解释三明治薄带GMI随外磁场方向变化特性. 相似文献
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J.K. Cheng Z.J. Zhao H. Lin Z.M. Wu X.L. Yang W.Z. Yuan 《Journal of magnetism and magnetic materials》2008
CuBe/Insulator/NiCoP composite wire was prepared by electroless deposition on an insulated CuBe core with a diameter of 90 μm. The conversion relationship between the magneto-impedance and effective magnetic permeability of the composite wire was derived from an energy conversion model. The evolution of the magnetic permeability and the giant magneto-impedance (GMI) effect were investigated. The results show that a distinct GMI effect can be obtained at relatively low frequency. The largest GMI ratio is 240% at 600 kHz, and the maximal field sensitivity is 34%/Oe. 相似文献
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Cytotoxicity and GMI bio-sensor detection of maghemite nanoparticles internalized into cells 总被引:1,自引:0,他引:1
F. Blanc-Béguin S. Nabily A. Turzo P.Y. Salaun 《Journal of magnetism and magnetic materials》2009,321(3):192-197
In this work we determine conditions to produce cell samples for imaging with detection of the modification of the magnetic field by maghemite (Fe2O3) nanoparticles acting as a high sensitivity magnetic bio-sensor based on the giant magneto-impedance (GMI) effect. Mat Ly Lu cells are grown for 24 h with various maghemite nanoparticles concentrations (from 0 to 6 mg/ml). The percentage of viable cells is determined by counting labeled cells with trypan blue under an optical microscope. The quantity of nanoparticles internalized into the cells is evaluated by X-ray fluorescence analysis and expressed in iron moles per cell. The GMI bio-sensor was tested with the various samples. We observed that the best sensitivity of the GMI bio-sensor was obtained at a frequency of 1 MHz. To confirm these results in the presence of cell samples, four measurement frequencies were pre-selected (from 1 to 100 MHz) and tested. Cell growth conditions compatible with an acceptable percentage of cell viability for various concentrations of nanoparticles were also determined. These experiments allow us to conclude that cell growth with 0.1 mg/ml of nanoparticles for 24 h shows modifications of the magnetic field detectable optimally at 1 MHz frequency. 相似文献
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《Journal of magnetism and magnetic materials》2001,234(3):359-365
The giant magneto-impedance (GMI) ratio, ΔZ/Z=[(Z(H)−Z(Hmax)]/Z(Hmax), in a nearly zero magnetostrictive Co68.5Mn6.5Si10B15 amorphous microwire has been investigated for the frequency range 0.5–10 MHz, driving current amplitude of 0.5–2.5 mA, bias DC magnetic field up to 2400 A/m and under applied tensile stress up to 132 MPa. A maximum relative change in the GMI ratio up to around 130% is observed at a frequency of 10 MHz, magnetic DC field of about 180 A/m, driving current amplitude of 1 mA and under tension of 60 MPa. The tensile stress dependence of the magnetic field, Hm, corresponding to the maximum ΔZ/Z ratio allows to estimate the magnetostriction constant (λs≈−2×10−7) to be in good agreement with λs values estimated by different methods and in amorphous alloys with similar compositions. 相似文献
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Giant magnetoimpedance (GMI) effect has been measured in a glass-coated amorphous (Co0.93Fe0.7)63Ni10Si11B16 microwire as a function of DC magnetic field and up to the frequency of 11 MHz. The sample shows single peak GMI characteristics within the whole range of frequency. The domain structure of the above sample has been changed by applying tensile stresses up to 603 MPa and current annealing with a DC current of 50 mA for various time durations, and the corresponding effect on GMI has been studied in detail. A maximum change of 8.85% in MI of the as-quenched sample has been observed around a frequency of 5.05 MHz. Application of an external tensile stress reduces the GMI value by increasing the inner core domain, whereas heat treatment of the sample enhances the same. The square-shaped magnetic hysteresis loop of the as-quenched sample helps us understanding the MI results. 相似文献