Gdx((Fe83Co17)55Ag45)100-x颗粒膜结构及巨磁电阻效应研究

复合靶以Fe,Co,Ag和Gd按一定比例组成,采用磁控溅射法制备了Gdx((Fe83Co17)55Ag45)100-x(x=0,3.5,5.0,6.5,8.0,9.5)颗粒膜。在室温下,利用X射线衍射仪(XRD)、四探针电阻测试仪、振动样品磁强计(VSM)等方法研究Gd的掺入以及不同退火温度对颗粒膜显微结构、巨磁电阻效应(GMR)和磁性能影响。X射线衍射实验结果表明:薄膜形成了以Ag(111)和FeCo(110)组成的合金结构,且增加稀土Gd的掺入量能促进薄膜基体中FeCo与Ag的相分离。磁电阻测试结果发现:不同成分的Gdx((Fe83Co17)55Ag45)100-x(x=0,3.5,5.0,6.5,8.0,9.5)薄膜样品均随着退火温度升高以及稀土Gd含量增加,颗粒膜巨磁电阻(GMR)效应呈现先增后减的趋势,且饱和场逐渐降低,当x=5.0、退火温度250℃时,Gd5.0((Fe83Co17)55Ag45)95.0薄膜巨磁电阻效应达到最大,GMR值为-14.8%。Gd掺杂后样品磁滞回线的变化表明薄膜的矫顽力较小,矩形比随Gd含量的增加而增加,分析认为Gdx((Fe83Co17)55Ag45)100-x薄膜具有良好的软磁性能。     

La2/3Ca1/3MnO3/xTiO2复合磁性材料的磁电特性研究

采用溶胶-凝胶法制备La2/3Ca1/3MnO3纳米级磁性颗粒和TiO2胶体,按一定比例制成La2/3Ca1/3MnO3/xTiO2(其中x取0、0.1、0.2、0.3、0.4)复合磁电阻材料。用XRD谱确定样品的晶体结构。采用振动样品磁强计测量了样品的磁滞回线和场冷却磁化强度随温度的变化行为;采用标准四引线法测量样品在恒定磁场下的电阻率随温度的变化。实验测量结果表明体系的磁化强度、剩磁、矫顽力随TiO2含量的变化具有相似的规律,具有室温的居里温度;并且当磁场强度小于0.4T时,磁电阻与磁场平方成正比关系;当大于0.6T时,磁电阻与磁场成线性关系。     

软磁金属合金多层磁性薄膜研究进展

概括介绍了金属软磁合金多层薄膜巨磁电阻效应和巨磁阻抗效应的研究和应用，对多层薄膜的制备方法和表征手段作了介绍。磁性金属多层薄膜的层间耦合的理论和模型也进行了介绍。重点是三明治结构、白旋阀结构及隧道结结构等多层膜。最后介绍了磁电阻磁头和磁传感器等应用情况和对该领域研究的展望。     

铁磁金属纳米点接触的磁电阻

分析三种不同方法制备的铁磁金属纳米点接触样品的弹道磁电阻现象,使用原子力显微镜准确测量铁磁金属点接触样品的磁致伸缩和微磁力行为,探讨由于磁致伸缩和微磁力等机械因素引起的样品微观结构变化对所测量铁磁金属纳米点接触样品的弹道磁电阻效应所产生的影响,得出在变化磁场作用下,在铁磁金属纳米点接触样品中所观察到的大比例弹道磁电阻现象可能与样品发生的微观结构变化而导致的电阻变化有关.     

纳米稀土铁氧体磁性颗粒的制备研究

采用湿化学方法研究制备纳米稀土铁氧体磁性颗粒，研究纳米稀土铁氧体颗粒制备过程中主要影响因素，如pH和RE^3＋等对纳米稀土铁氧体颗粒粒径及磁性能的影响；同时对纳米Dy铁氧体颗粒的形貌、粒度分布、晶型结构及磁性能进行了分析和研究。研究发现轻稀土对Fe3O4颗粒的磁性有削弱作用，不宜掺杂；重稀土元素掺杂是提高铁氧体磁性颗粒磁性能的有效途径，改善磁性能的强弱顺序为Dy^3＋〉Gd^3＋〉Er^3＋。制备的Dy铁氧体颗粒的平均粒径为9．6nm，比饱和磁化强度98．27A·m^2·kg^-1，具有超顺磁特性。同时讨论了Dy^3＋在Fe3O4的晶体结构中取代Fe离子增强磁性能的可能形式。     

改善钙钛矿材料室温下磁电阻效应的有效途径

将Ag2O与La0.67Ca0.25Sr0.08MnO3均匀混合经高温烧结后形成La0.67Ca0.25Sr0.08MnO3/xAg两相复合体系。随Ag掺入量的增加,样品的电阻率明显下降,磁化强度有小量下降,TC及电阻率的峰值温度TP没有明显变化。304K温度下,从x=0.25样品中得到最大磁电阻效应,磁电阻比约为41%,分别是La0.67Ca0.25Sr0.08MnO3和La0.67Sr0.33MnO3样品的1.6及10倍。磁电阻的本征效应和传导电子在界面处的自旋相关散射作用是产生室温下增强磁电阻效应的主要原因。结果说明,利用离子的掺杂效应调整居里温度到室温附近,再结合金属/钙钛矿复合体系界面属性丰富的特性来制备庞磁电阻材料是提高室温磁电阻有效的途径,这对应用研究具有十分重要的意义。     

Cu_x(Al_2O_3)_(1-x)颗粒膜的巨霍耳效应研究

在由磁性金属颗粒镶嵌在非磁金属或绝缘基体中而形成的两相非均匀颗粒系统中 ,当磁性金属的体积百分含量处于临界值时 ,体系的输运行为有许多奇异的现象。相继在在磁性金属 非磁金属和磁性金属 绝缘体系统中发现了巨磁电阻效应和隧道磁电阻效应 ;特别的在磁性金属 绝缘体系统中发现了反常霍耳效应的极大增强 ,称为巨霍耳效应。为了探讨颗粒体系的巨霍耳效应的机制 ,本文用离子束共溅射的方法制备了大约 1.5× 10 - 7m厚度的Cux(Al2 O3) 1 -x颗粒薄膜 ,研究了非磁金属 绝缘体体系 :Cu Al2 O3颗粒系统的巨霍耳效应 ,发现在量子渗流阈值时 ,霍耳电阻比正常金属高 2个数量级。     

纳米材料的巨磁电阻效应及其应用

综述了纳米巨磁电阻材料的最新研究进展,主要包括多层膜、颗粒膜、纳米颗粒合金薄带,隧道结、钙钛矿结构等的性能、机理、制备、研究方向和应用。     

Cux(Al2O3)1-x颗粒膜的巨霍耳效应研究

在由磁性金属颗粒镶嵌在非磁金属或绝缘基体中而形成的两相非均匀颗粒系统中, 当磁性金属的体积百分含量处于临界值时, 体系的输运行为有许多奇异的现象. 相继在在磁性金属/非磁金属和磁性金属/绝缘体系统中发现了巨磁电阻效应和隧道磁电阻效应; 特别的在磁性金属/绝缘体系统中发现了反常霍耳效应的极大增强, 称为巨霍耳效应. 为了探讨颗粒体系的巨霍耳效应的机制, 本文用离子束共溅射的方法制备了大约1.5×10-7 m 厚度的Cux(Al2O3)1-x颗粒薄膜, 研究了非磁金属/绝缘体体系Cu/Al2O3颗粒系统的巨霍耳效应, 发现在量子渗流阈值时, 霍耳电阻比正常金属高2个数量级.     

电沉积制备铜钴颗粒膜

采用电沉积方法制备了铜钴巨磁电阻功能膜，研究了电沉积工艺参数，包括镀液的主盐离子浓度、配合剂浓度、pH值以及沉积时的电流密度等对铜钴颗粒膜层的组成的影响．用扫描电镜、金相显微镜、EDX能谱仪和XRD分析了镀层组成、表面形貌和结构．膜层的组成成分、晶粒大小与镀液的主盐离子浓度、配合剂浓度、pH值以及沉积时的电流密度有着直接的联系．镀液中钴离子浓度增大时，镀层中的钴含量相应的提高，镀层结晶更加粗大．镀层中铜离子浓度增大时，镀层中的铜含量提高，镀层结晶变得致密．配合剂柠檬酸钠浓度增加对镀层中钴的含量起到一定的抑止作用，而对铜的沉积则有促进作用，同时颗粒膜层结晶更加致密．低pH值下有利于铜的沉积，但此时镀层的晶粒较为粗大．控制电流密度可以改变镀层的组成，较高的电流密度有利于钴的沉积．     

Rare-Earth Functional Films Prepared by Ion Beam Epitaxy

Rare-Earth Functional Films Prepared by Ion Beam Epitaxy     

Polymer Bonded Anisotropic Thick Hard Films for Micromotors/Microgenerators

Hard magnetic films are very promising elements for the production of MEMS, due to the optimum scaling properties of magnetic interactions. These elements are specially well suited for the development of micromotors and microgenerators. A magnetization multipolar structure is required on the material to be used in such applications. In order to generate this multipolar structure, a well defined magnetic anisotropy is required, this anisotropy being directed in many cases in the direction perpendicular to the film plane. The maximum torque obtainable from a micromotor depends mainly on the mass of magnetic material (i.e. the film thickness). Anisotropic hard magnetic films with thicknesses on the order of tenths of millimetres can not be prepared by any of the common thin film deposition techniques available nowadays. Though some preparation techniques have been developed that can be used to prepare hard magnetic films with the desired thicknesses, they are not able to produce materials with a well defined anisotropy along the direction perpendicular to the film plane. In this work, we describe a method to prepare anisotropic hard magnetic films with thicknesses of tenths of millimetres by dispersing NdFeB anisotropic microparticles on a polymethyl methacrylate (PMMA) solution at room temperature under low intensity magnetic fields. Large macrospic anisotropics have been reached for magnetic fields as low as 150 Oe applied during the deposition, with room temperature coercivities in excess of 1.2 T and maximum energy products up to 9 MGOe. The analysis of the temperature dependence of the magnetic properties indicates that a columnar arrangement of the particles on the direction parallel to the field applied during the preparation is the reason of the observed macroscopic anisotropy. The films can be easily deposited onto different substrates and mechanised in order to obtain a smooth surface with the desired shape. Their use in micromotors/microgenerators has been tested.     

碳包覆磁性金属纳米胶囊的制备及表征

采用直流电弧等离子体法制备出表面包覆碳膜的金属纳米颗粒,这种纳米颗粒通常被称为“纳米胶囊”。其表面包覆气密的碳膜,具有良好的抗氧化性和稳定性。在甲烷气氛中蒸发各种磁性金属可获得具有良好物理化学性能的磁性纳米胶囊。对这种纳米胶囊进行了Ｘ射线衍射、Ｘ光电子谱、俄歇能谱、氧含量测定及ＨＲＴＥＭ、磁性分析等研究,提供了确定纳米颗粒新型壳－核结构的可靠实验依据。     

Magnetic Properties and Kinetics Parameters of Electroless Magnetic Loss CoFeB Films

Electroless CoFeB films with good soft magnetic properties were fabricated on polyester plastic substrate from sodium tartarate as a complexing agent.The plating rate of electroless CoFeB films is a function of concentration of sodium tetrahydroborate,pH of the plating bath,plating temperature and the metallic ratio.The estimated regression coefficient b0-b3 confidence interval,residual error r and confidence interval rint were confirmed by a computer program.The optimal composition of the plating bath was obtained and the dynamic electromagnetic parameters of films were measured in the 2-10 GHz range.At 2 GHz,the μ＇,μ″ of the electroless CoFeB films were 304 and 76.6,respectively,as the concentration of reducer is 1 g/L.Magnetic hysteresis loop of the deposited CoFeB films show a remanence close to the saturation magnetization and coercivity of about 55.7-127.4 A/m.The loops along the hard axis display low anisotropic field Hk of 2 388-3 582 A/m.     

Anisotropic Magnetoresistance of Perovskite La_(2/3)Ca_(1/3)MnO_3/YBa_2Cu_4O_8/La_(2/3)Ca_(1/3)MnO_3 Trilayer Films

Magneticanisotropyhasbeenfoundinmanyex oticmaterials,suchasmetallicsuperlatticeswithgi antmagnetoresistanceeffectsandthehightempera turesuperconductingoxideYBa2Cu3O7 δ[1～4].The anisotropycouldfindnovelusesinnewdeviceappli cations.Agoodexampleisthehig…     

Preliminary evaluation of an SF5+ polyatomic primary ion beam for analysis of organic thin films by secondary ion mass spectrometry

Organic vapor deposited thin films of pure biomolecules, polymer films and biomolecules dispersed in gelatin and biological tissue have been analyzed in a magnetic sector secondary ion mass spectrometer using an SF5+ primary ion beam at keV impact energies. In comparison to Ar+ bombardment under identical conditions, bombardment with SF5+ gives a 10 to 50 fold enhancement in the secondary ion yields for characteristic molecular ions. The SF5+ primary ion beam can be focussed to a small spot allowing molecular ion images to be obtained at micrometer spatial resolution with enhanced sensitivity. More importantly, the decay in molecular ion signal as a function of primary ion dose commonly observed in SIMS using monoatomic primary ions is either eliminated or greatly reduced, allowing molecular depth profiles to be obtained of organic thin films. By continuing to sample intact molecules as sputtering proceeds into the sample, the total number of detected characteristic secondary ions is increased by as much as a factor of approximately 700 for SF5+ bombardment as compared to Ar+ bombardment under identical analytical conditions. This effect is thought to be a result of the high erosion rate and the low penetration depth inherent in the use of a polyatomic primary projectile.     

Magnetic anisotropy induced in the nanocrystalline FeZrN films prepared by oblique-angle magnetron sputtering

Nanocrystalline Fe₇₇Zr₇N₁₆ films are prepared by oblique-angle magnetron sputtering. The effect of the ion beam angle and subsequent annealing on the phase and structural states, the coercive force, the saturation magnetization, the remanent magnetization, and the induced in-plane magnetic anisotropy field has been studied. The possibility of natural ferromagnetic resonance in these films at gigahertz frequencies is estimated.     

加剂方式对烧结钕铁硼磁体磁性能的影响

钕铁硼永磁材料在民用、航空航天等众多领域得到广泛的应用.高档次烧结钕铁硼磁体具有良好的市场前景.商业磁体多是由大块烧结毛坯切割而成,磁性能一致性是市场的基本要求之一,润滑剂等化学试剂和磁粉混合不均匀是影响一致性的一个重要因素.钕铁硼磁粉化学性质活泼、容易氧化,制粉的全过程都在氮气气氛下进行,没有合适的设备,想均匀加入化...     

Study on Magnetic Responsibility of Rare Earth Ferrite／Polyacrylamide Magnetic Microsphere

Magneticpolymermicrospherecanbeseparatedquicklyundermagneticfieldandithasgotwideappli cationinmanyfields ,suchascellseparationetc .Themicrospheremustpossesshighmagneticresponsibili ty ,sothatmagneticseparationisquickandconve nient.Themagneticresponsibilit…     

Effects of Hydrogen Ion Implantation on TiC-C Coating of Stainless Steel

Titanium carbide coatings are widely used as various wear-resistant material.The hydrogen erosion resistance of TiC-C films and the effect of hydrogen participation on TiC-C films were studied.Seventy-five percent TiC-C films are prepared on stainless steel surface by using ion mixing,where TiC-C films are deposited by rf magnetron sputtering followed by argon ion bombardment.The samples are then submitted to hydrogen ion implantation at 1.2×10-3 Pa.Characterization for the 75% TiC-C films was done with SIMS,XRD,AES,and XPS.Secondary ion mass spectroscopy (SIMS) was used to analyze hydrogen concentration variation with depth,X-Ray diffraction (XRD) was used to identify the phases,and Auger electron spectra (AES) as well as X-ray photoelectron spectra (XPS) were used to check the effects of hydrogen on shifts of chemical bonding states of C and Ti in the TiC-C films.It is found that TiC-C films on stainless steel surface can prevent hydrogen from entering stainless steel.