巨磁电阻效应实验仪

自制了巨磁电阻效应实验仪,测量了不同外磁场和工作电压下巨磁阻传感器输出电压的变化.研究了巨磁阻传感器敏感轴与外磁场间夹角与传感器输出电压间关系,传感器输出电压的与偏离角度成余弦关系.     

巨磁电阻效应实验仪的研制与应用

阐述了巨磁电阻效应实验原理、实验内容和实验方法,该仪器可测量巨磁电阻阻值与磁感应强度关系,并与正常磁电阻、坡莫合金磁电阻特性进行比较,仪器还提供巨磁电阻传感器特性测量及系列应用实验供教学使用.     

掺杂稀土锰氧化物的巨磁电阻效应

介绍了掺杂稀土锰氧化物的巨磁电阻效应研究概况和最新进展，在综合目前实验和理论研究结果的基础上，对在掺杂稀土锰氧化物材料中引起巨磁电阻效应的物理机制进行了探讨，对这一材料的应用前景和需要做的工作进行了讨论。     

纳米微粒系统中的巨磁电阻效应

重点介绍含有铁磁纳米微颗粒系统中的巨磁电阻效应，例如颗粒膜，快淬纳米复相固体居磁电阻效应与铁磁组成，颗粒尺寸，形状的依赖性。     

纳米材料中的巨磁电阻效应

纳米材料是指三维空间尺度中至少有一维处于纳米量级的材料，通常为１—１００ｎｍ，如纳米微粒，纳米线、管，纳米薄膜或其组合材料，近年来纳米材料中的巨磁电阻效应颇受人们青睐，本文将重点介绍颗粒膜，颗粒合金薄带，非连续多层膜，颗粒—薄膜混合型膜以及磁性隧道结的巨磁电阻效应。     

磁性多层薄膜系统中的巨磁电阻效应

考虑到量子尺寸效应以及来自杂质、粗糙表面、粗糙界面三方面的散射,运用量子统计格林函数方法和久保理论,计算了磁性多层薄膜系统中的巨磁电阻,讨论了巨磁电阻随非磁层厚度作周期性振荡,以及在(Fe/Cr)_N/Fe系统中巨磁电阻随多层基元数目N增加而增大等现象.理论计算与实验结果符合.此外,还讨论了有关各种散射引起的散射率能否相加的问题. 关键词：     

基于巨磁电阻效应的多功能测量仪

利用巨磁电阻传感器设计了多功能测量仪器,实验表明该测量仪能够精确测量物体的转速和转角,直观地演示行驶车辆对地磁场的扰动.     

金属颗粒薄膜巨磁电阻效应的影响因素

研究金属颗粒薄膜的颗粒尺寸、磁性组分等对巨磁电阻效应的影响.在自由电子模型和自旋相关散射理论的基础上，计算了金属颗粒膜体系的电子平均散射势.在计算过程中将自旋相关项与宏观量相联系，得到了巨磁电阻效应与磁性成分比例、颗粒尺寸的关系.磁电阻效应的模拟曲线表明，增加磁性成分比例和减小磁性颗粒尺寸可增强颗粒膜的巨磁电阻效应. 关键词：     

具有室温巨隧道磁电阻效应与高自旋极化率的新材料

回顾了隧道磁电阻效应发展简史及其应用，报道了锌铁氧体／氧化铁二相纳米复合材料在室温具有巨磁隧道电阻效应的实验结果，该实验结果表明锌铁氧体是具有高自旋极化率的一类新材料，值得进一步开展相关的研究工作。     

Fe-Al2O3颗粒膜的隧道巨磁电阻效应

对射频共溅射法制备的ＦｅＡｌ２Ｏ３颗粒膜的隧道巨磁电阻效应进行了研究．当Ｆｅ体积百分比为４５％时,样品的室温磁电阻的变化率（ＭＲ）在１Ｔ的平行膜面的磁场下可达４４％．磁测量表明在室温时样品呈超顺磁态．另外,从ＭＲ随温度的变化关系曲线可以看出,当温度低于５０Ｋ时,ＭＲ随着温度的下降而显著增加,ＭＲ在２０Ｋ时达到１４９％,４２Ｋ时可达２６％,大大超过理论的预期值,这可能与低温下由库仑抑制效应引起的自旋相关隧穿的高阶效应有关．     

Conductance of highly oriented pyrolytic graphite nanocontacts

The conductance-voltage G(V) characteristics for contacts between electrodes of highly oriented pyrolytic graphite were studied in a wide range of G(0), bias voltages, and temperatures using the mechanically controllable break junction technique. Our results show a striking resemblance to corresponding data for conducting multiwall carbon nanotubes. For high-ohmic contacts between a single or a few graphene sheets, zero bias anomalies related to strong e–e Coulomb interactions and quantum interference of electrons is observed. PACS 72.15.-v.; 72.80.Rj; 73.63.Rt     

Two-dimensional spectral-spatial image of highly oriented pyrolytic graphite

Experimentally observed electron paramagnetic resonance (EPR) spectra of highly oriented pyrolytic graphite samples can be considered as a sum of three signals coming from two adjacent faces and crystal edges. Contributions from faces can be analyzed analytically by Dyson’s theory based on an infinite flat conductive plate, while the contribution from edges is not described by this theory. Overlapping of these signals makes it difficult to get useful information about the sample from spectra observed. Implementation of two-dimensional spectral-spatial imaging technique proved to be helpful to solve this problem. It permits the characterization of the EPR spectrum from a selected flat spatial region located far from crystal edges where the model of the infinite flat conductive plate can be applied. By analyzing the EPR signal from spatial slices by Dyson’s equation we have obtained the values of the diffusion coefficient and the surface relaxation rate.     

Visualization of human plasma fibrinogen adsorbed on highly oriented pyrolytic graphite by scanning probe microscopy

Human plasma fibrinogen (HPF) was observed by atomic force microscopy (AFM) and Kelvin probe force microscopy (KPFM) conducted in non-contact mode. The HPF was adsorbed on a highly oriented pyrolytic graphite (HOPG) substrate as single molecules, as aggregated bundles, and as aggregated fibers. Topographic and phase images confirmed structural changes in the HPF after exposure to air, while topographic and KPFM images confirmed fibers with the width of a single HPF molecule. Additionally, KPFM confirmed the surface potential difference between the HPF and the HOPG, and periodical potential drop reflecting the E and D domains in the fiber.     

VUV photochemistry of oriented molecules: methylchloride on highly oriented pyrolytic graphite

The photoionization of CH₃Cl adsorbed on highly oriented pyrolytic graphite has been investigated as a function of the photon energy in the range 13–35 eV. Two ions were detected — CH⁺₃ and H⁺ — which show differences in their coverage and energy dependences. At very low coverages only H⁺ ions are produced, while at higher coverages (still in the monolayer regime) CH⁺₃ ions are also observed, reflecting a change in the orientation of the molecule on the surface as a function of coverage. The cross-section curves as a function of the photon energy for both ions show a maximum at 22 eV, while the onsets are at 16 eV for CH⁺₃ and 19 eV for H⁺.     

Effects of Mn doping on BaTiO3 thin films grown on highly oriented pyrolytic graphite substrates

We report multiferroelectric properties of Mn-doped BaTiO₃ (MBTO) thin films on highly oriented pyrolytic graphite (HOPG) substrates. The MBTO thin films were grown on the HOPG substrate by pulse laser deposition. For comparison purpose, undoped BaTiO₃ (BTO) thin films were also prepared under same experimental conditions. The BTO and MBTO thin films were polycrystalline, indicating that the MBTO thin film has better crystallinity than the BTO thin film. The leakage current of the MBTO thin film was reduced due to the Mn doping substitution. In addition, the MBTO thin film exhibited better than the BTO thin film in ferroelectric and magnetic behaviors. We suggest that the Mn doping bring about the improvements of ferroelectric and ferromagnetic properties of the BTO thin films. Based on atomic force microscopy (AFM) and conducting AFM (CAFM) studies, the grain size of MBTO thin film was much larger than that of BTO thin film.     

高定向热解石墨表面局域导电增强现象的扫描探针显微学研究

基于导电型原子力显微镜和扫描隧道显微镜的对比观察,研究高定向热解石墨表面上残留石墨片的导电增强现象.根据样品电阻的测量数据,将这种现象归结为导电针尖与石墨表面的点接触问题,并且发现接触电导和接触点处局域的电子密度成正比,从而确定石墨表面的局域导电增强现象的原因在于残留在石墨表面的石墨片具有较高的电子密度. 关键词： 扫描隧道显微镜 导电原子力显微镜 高定向热解石墨 导电性     

Effects of the deep ion-induced modification of highly oriented pyrolytic graphite

The capabilities of in situ ion-electron emission monitoring of the effects of deep modification for surfaces of highly oriented pyrolytic graphite at high ion irradiation fluences and determining the threshold radiation damage level of these effects are demonstrated experimentally.     

Sputtering of highly oriented pyrolytic graphite with 30 keV Argon ions

The influence of the incidence angle of 30 keV Ar⁺ ions, ion fluence and target temperature on the sputtering yield and surface microgeometry of highly oriented pyrolytic graphite (UPV-1T) samples was experimentally studied. It was found that at fluences more than 5 × 10¹⁹ ion cm^?2 the sputtering yield at room temperature in the range of the ion incidence angle from 0° to 80° is twice as small as the corresponding experimental data for both polycrystalline graphite and glassy carbon. The analysis of ion-induced relief permits us to suppose the topographical suppression mechanism of highly oriented pyrolytic graphite sputtering.     

Simultaneous observation of the triangular and honeycomb structures on highly oriented pyrolytic graphite at room temperature: An STM study

Scanning tunneling microscopy (STM) was used to study the surface structures of dry-prepared and di-chloroethane-treated HOPG samples. Both triangular and honeycomb structures were simultaneously observed with the same tip at room temperature around a strand (grain boundary) on the HOPG surface. This observation did not support the tip effect in STM imaging explanation for HOPG in literature. A general layer-sliding model was utilized to explain the experimental results: sliding of the HOPG topmost layer was used to explain the origins of the triangular and honeycomb structures, and molecule intercalation into inter-layer spacing between the first and second layers of HOPG induced inhomogeneous deformation of the HOPG topmost layer that accordingly generated the Moiré patterns of the HOPG sample in di-chloroethane.     

An artefact in scanning tunneling microscopy images of highly oriented pyrolytic graphite

An artefact with a structure that appears as an ordered array of chains, several 1000 Å long and with distances of between 10 Å and 30 Å in STM images of HOPG is reported. The artefact, which emerges from a too low point density in the scanning grid during data aquisition in the scanning tunneling microscope, is explained using the atomically resolved image, the orientation of the substrate in the STM, the sequential character of data acquisition in scanning tunneling microscopy together with the limited number of data points for the reconstruction of STM images and related image-processing problems, and the specific noise spectrum of the tunneling current. The identification of the artefact is verified by a computer simulation of the STM images, which reproduces the experimental data in detail.