双层钙钛矿Sr2FeMoO6，Ba2FeMoO6的电磁性质研究

分析了双层钙钛矿结构的锰氧化合物Sr2FeMoO6,Ba2FeMoO6物相结构和电磁学性质,对巨磁阻效应进行了探讨,揭示了Sr2FeMoO6样品为半导体导电性,Ba2FeMoO6样品为金属导电性.     

快淬CoNiCu系列金属条带的巨磁电阻效应

研究了用快淬制备的铸态和退火处理后的颗粒合金膜Co 20NixCu 80-x(0≤x≤20)的结构、磁电阻性能.利用电镜观察到Co-Ni纳米颗粒在Co-Ni-Cu合金薄膜中分布均匀,与Co-Cu合金薄膜有不同.CoNiCu系列样品随Ni成分的增加,其相变过程由形核长大类型向失稳分解类型过渡.而且在室温下有比Co-Cu样品有更大的MR幅度.750 K下退火10 min的Co 20Ni5Cu 75快淬条带在300 K下的ΔR/R≌6.5%.     

M-M型纳米颗粒膜的巨磁电阻效应

探讨了M-M型纳米颗粒膜巨磁电阻效应的物理机制，指出了影响颗粒膜巨磁电阻效应的因素，推导出M-M型纳米颗粒膜巨磁电阻效应的计算公式。     

高分辨率磁旋转编码器磁鼓材料的研制

采用磁浆涂布工艺制作了磁鼓涂层材料.研究了不同组分的配方对磁鼓涂层材料性能的影响,制备出性能良好的磁鼓.对Φ32～40mm的磁鼓进行了充磁测试,写入了128和256对极.采用金属薄膜磁电阻传感探头检测磁鼓表面分布磁场,信号通过电路放大、整形后接入示波器和计数器,结果显示输出信号波形良好,计数完整.     

非磁金属中间层对磁性隧道结磁电阻效应的影响

用自由电子近似方法对具有非磁金属中间层的磁性隧道结的磁电阻进行了研究，从理论上讨论了非磁金属中间层对磁电阻的影响。数值计算结果表明，当外加偏压不同时非磁金属中间层的作用是不同的。在外加电压使电子从非磁金属中间层穿过势垒的情况下，非磁金属中间层的变厚可以增强隧穿磁电阻效应。这一性质可以用于磁性隧道结的优化。     

巨磁电阻效应

重点综述了磁性多层膜、颗粒膜、钙钛矿型氧化物及铁磁薄膜隧道结等几种不同结构类型的巨磁电阻效应的研究现状及其进展情况,并简述了巨磁电阻的物理机制及磁传感器、随机存储器和高密度读出头等几方面的应用,还涉及到了制备这些巨磁电阻材料的常用方法,并列举了10种不同组分的巨磁电阻材料,还说明了特大磁电阻和巨磁电阻的不同。     

低饱和场巨磁电阻金属多层膜Ni80Fe20／Cu的结构与磁电阻

采用磁控溅射方法，获得了具有低饱和场巨磁电阻的Ｎｉ８０Ｆｅ２０／Ｃｕ金属多层膜，在室温下，其磁电阻和层间耦合状态随Ｃｕ层厚度的增加呈振荡变化，在Ｃｕ层厚度ｔＣｕ＝１．０ｎｍ，２．２ｎｍ时磁电阻出现２个峰值分别为１９．４％和１１．７％，饱和场约为６．４×１０＾４Ａ／ｍ和８×１０＾３Ａ／ｍ低温下（７７Ｋ）磁电阻为３３．２％和２７．６％，系统地研究了ＮｉＦｅ层厚度和周期数对多层膜磁电阻的影响，用真空退火     

Magnetoresistance of the thin film ferromagnetic nanoconstrictions

The magnetoresistance and I-V characteristics at different temperatures of the thin film ferromagnetic nanoconstrictions of variable width (from 20 to 250 nm) and 10 nm thicknesses, fabricated by electron beam lithography and vacuum thin film deposition are compared. The magnetoresistance and resistance of the thin film ferromagnetic nanoconstrictions are not related to the width of the nanoconstrictions. Instead the resistance of the local nano-region in the middle of the thin film ferromagnetic nanoconstriction has only a minor role compared to that of the two microscale thin film ferromagnetic electrodes, which contribute the majority of the measured resistance. The magnetoresistances of the thin film ferromagnetic nanoconstrictions and a 0.2 cm × 0.8 cm thin ferromagnetic film deposited under the same conditions were also compared; the thin film ferromagnetic nanoconstrictions have higher magnetoresistances than the thin ferromagnetic film, which implies that the measured magnetoresistance of the thin film ferromagnetic nanoconstrictions comes mainly from the local nano-region in their centers. In conclusion, the measured magnetoresistance of the whole sample is similar to the anisotropic magnetoresistance, because the resistance of the two microscale thin film ferromagnetic electrodes is much higher than that of the local nano-region in the middle of the samples. Comparing the experimental results for the thin film ferromagnetic nanoconstrictions and the thin ferromagnetic film reveals that the magnetoresistance of the local nano-region in the middle of the sample is much higher than that of the two microscale thin film ferromagnetic electrodes attached to it.