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1.
2.
The grain growth dependence of microstructure and its effects on magnetic and transport properties are studied in the polycrystalline La0.67Ba0.33MnO3 oxides. It is found that a lateral growth manner along a certain direction and a concentric terrace pattern along three orthogonal axes occur in the samples sintered at 1573 and 1673 K, respectively. Lamella-like twin microstructure forms in the concentric terrace growth pattern and the magnetoresistance properties can be enhanced by the twin microstructure. It suggests that the twin-boundaries in twin-grains may possibly induce spin-dependent scattering of electrons that is field reduced, or spin-polarized tunneling of electrons that is field enhanced, thus strengthening the effect of grain boundaries.  相似文献   

3.
Magnetic hysteresis properties of antiferromagnetically exchange-coupled bilayer structures, in which the two magnetic layers have different magnetic parameters and thicknesses, are studied within the framework of the Stoner-Wohlfarth model. Analytical expressions for the switching fields corresponding to the linear magnetic states are obtained. By adjusting the magnetic parameters or thicknesses of layers, nine different types of easy-axis hysteresis loops may exist. The phase diagram of easy-axis hysteresis loops is mapped in the k1 and k2 plane, where k1 and k2 are the ratios of magnetic anisotropy to the interlayer exchange coupling of the two magnetic layers, respectively.  相似文献   

4.
We report a novel bi-layer thin film structure for high density magneto-optical (MO) data storage, which combines the advantages of blue wavelength and magnetically induced superresolution (MSR) recording. A double-layer system of exchange-coupled light rare-earth (LRE) element doped NdGdFeCo and traditional TbFeCo is used as the recording medium. The experimental results demonstrate that this NdGdFeCo/TbFeCo double layer has large Kerr rotation under blue wavelength. Centre aperture detection (CAD) MSR effect with temperature rising is also observed. Theoretical calculation is also carried out to verify the experimental results. These results collectively suggest that the new bilayer structure is very promising in next generation high density MO data storage.  相似文献   

5.
    
The influence of annealing on giant magnetoresistance (GMR) effect and magnetization reversal processes has been investigated in Py/Cu (Py = Ni83Fe17) sputter‐deposited multilayers (MLs) with a limited number of magnetic sublayers (N ≤ 6) and equal sublayer thicknesses both for Py and Cu (tCu = 2 nm, tPy = 2 nm). Based on the magnetization and magnetoresistance measurements it has been shown that the magnetic behavior of such MLs is strongly influenced by annealing driven disruption of magnetic layers (lateral decoupling) and nonmagnetic layers (magnetic bridging between Py layers). A comparison of experimental hysteresis curves with model dependences indicates that annealing causes a change of the magnetization reversal from a local to an absolute energy minimum mode leading to quasi‐two‐state magnetoresistance characteristics.  相似文献   

6.
    
Top and bottom pinned spin valve structures have been fabricated using rf magnetron sputtering to study the depth sensitive exchange coupling. M‐H curves of both the configurations in as‐deposited and annealed forms have been measured by vibration sample magnetometry (VSM) and transverse Kerr effect spectrometry (TKE) using DC and AC magnetic fields, respectively. The TKE signal was also examined as a function of wavelength in the range from 300‐800 nm, to obtain data from the full length of the bottom NiFe free layer covering either side of the interface. Annealing of the samples brings in higher values of exchange bias field compared to as‐deposited samples perhaps due to improved uniformity in exchange conditions. The TKE data at 500 nm wavelength point towards energetically favourable spin structure at the pinned interface. Wavelength dependence of the TKE data shows an anamolous trend close to the NiFe‐Cu (seed layer) inteface, which was attributed to a periodic Cu diffusion assisted non‐specular reflection (diffraction) component. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

7.
    
Magnetic properties of a patterned micro‐NiFe element were analyzed with micro‐MOKE and micromagnetics. Patterned 8 μm × 16 μm NiFe elements have higher coercive field, Hc = 1.9 Oe, for the hard axis than that, Hc = 0.2 Oe, of a 5 mm diameter disk NiFe sample. The magnetization reversal processes have been investigated with the micromagnetic simulation for the various applied field directions. The increase of coercive field in patterned micro‐NiFe elements can be attributed to the large shape anisotropy and pinned spins along the edges. Total anisotropy of a 8 μm × 16 μm NiFe sample was about 50 Oe. The magnetization reversal field of pinned spins along the edges in patterned micro‐NiFe sample was about 500 Oe. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

8.
    
Permalloy (Py)/capping (FeMn, Ta) bilayers with interconnected network structure were deposited onto porous alumina templates with 5.0 nm thick Ta buffer layers. For the nanostructured Py/FeMn and Py/Ta bilayers the coercivity goes through a maximum value near the Py layer thickness of 17.5 nm. Despite exchange biasing, however, the coercivity of the former bilayers is smaller than that of the latter ones with the same Py layer thickness. The Ta capping layer thickness and the deposition rate of the Py layer are also found to have great influences on the coercivity of the Py layer. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

9.
The temperature dependence of the saturation magnetization of a series of ionimplanted YIG films is presented. The films were implanted with neon ions at an energy of 450 keV; the dose ranged from 2 to 5*1014 ions/cm2. The experimental data can be described by the molecular field theory showing that the ion-implanted part of the film can be approximated as consisting of two regions each having their own magnetization and Curie temperature. The values of these magnetic parameters vary as a function of dose and differ strongly from the values for pure YIG.  相似文献   

10.
The magnetic microstructures and magnetotransport properties in granular CoxAg1-x films with 17%≤x≤62% were studied. Magnetic force microscopy (MFM) observations showed the presence of magnetic stripe domains in as-deposited samples with x≥45% and the evolution of the magnetic domain patterns to in-plane domains with annealing. A perpendicular magnetic anisotropy as high as about 8×105 ergs/cc for as-deposited Co62Ag38 and about 6×105 ergs/cc for as-deposited Co45Ag55 was observed by magnetization and torque measurements. With increasing annealing temperature, the perpendicular magnetic anisotropy became negative. The origin of the perpendicular magnetic anisotropy may be attributed to a rhombohedral distortion of the cubic cell due to residual substrate-film stresses. The magnetic stripe domains are the consequence of the interplay of the indirect or direct exchange, perpendicular magnetic anisotropy and dipolar interactions. Finally, magnetoresistance (MR) curves displayed training behaviours and different shapes when measured with different configurations (parallel, transverse and perpendicular). It is proposed that the existence and the evolution of the magnetic domain structures strongly affect the magnetotransport properties due to the extra contribution of the electron scattering at the domain walls. Furthermore, an anisotropic MR also contributes to the overall MR curves. Received: 2 March 2000 / Accepted: 28 March 2000 / Published online: 23 May 2001  相似文献   

11.
Transparent pure and Fe-doped SnO2 thin films were grown by pulsed laser deposition technique on LaAlO3 substrates. X-ray diffraction shows that the films are polycrystalline and have the rutile structure. Surprisingly, the pure film presents magnetic-like behavior at room temperature with a saturated magnetization of almost one-third of the doped film (∼3.6 and 11.3 emu/g, respectively) and its magnetization could not be attributed to any impurity phase. Taking into account the magnetic moment measured in the pure film, the effective contribution of the impurity in the doped one can be inferred to be ∼2 μB per Fe atom. A large magnetic moment was also predicted by an ab initio calculation in the doped system, which increases if an oxygen vacancy is present near the Fe impurity.  相似文献   

12.
Using the high spin asymmetry in inverse photoemission of the Ni d-band just above the Fermi level as an indicator of surface magnetization, we have measured hysteresis curves of the (110) surface of nickel. Nearly rectangular hysteresis loops indicate a well-defined behavior of the surface magnetization of the picture-frame single crystal with sides along 110 directions. The influence of geometrical order and chemisorption of O, S, and CO on the shape of the hysteresis loops has been investigated. We found a significant reduction of the coercive force (about 10%) if the clean high-quality (110) surface is disordered on an atomic scale by ion bombardment or low-coverage chemisorption.  相似文献   

13.
Two resonance modes occur when the magnetic spectra of rectangular ferromagnetic particles with different aspect ratio are studied using micromagnetic simulation. The intensity of the higher mode is stronger when the particles have the aspect ratio larger than 1.6. When the aspect ratio reduces to 1.6, only one strong resonance peak remains with some tiny satellite peaks appeared. These behaviors are attributed to the competition between the exchange interaction and dipolar coupling, which has different result in the edge and middle part, respectively.  相似文献   

14.
    
Metallic multilayers comprising ferromagnetic layers with different coercivities are of interest for magnetic sensor applications. Our purpose is to analyze the effects of interlayer coupling and number of interfaces between layers on the magnetic behavior of [Ni/Co—Ni—Mg—N] × n multilayers. The number n of periods varied from 1 to 52 for a total multilayer thickness of 1.5 μm. The multilayers were deposited onto a copper wire in an electrolytic cell system with a magnetic field Hd externally imposed during electroplating. The magnetic susceptibility curves obtained by induction method using a digital scope interfaced to computer were analyzed by real‐time Fast‐Fourier‐Transform (FFT) analysis. The magnetic behavior is explained by the complex internal magnetic configuration of the samples.  相似文献   

15.
We consider a model for magnetic memory that consists of strongly coupled dipolar or antiferromagnetic (AF) pairs with inequivalent perpendicular anisotropy K1K1 and K2K2. For appropriate parameter values, determined in this work, they have two inequivalent storage states with zero net magnetic moment. Both analytical and numerical calculations are performed, in some cases yielding different results because of relaxation effects (i.e., a dependence on the damping parameter αα). Hysteresis loops for a wide variety of parameter values are obtained, both for the AF case and the dipole case. An Appendix gives analytic results for slightly non-collinear spins in an applied field, which were used to test the numerical results.  相似文献   

16.
Based on both the spin diffusion equation and the Landau-LlTshitz-Gilbert (LLG) equation, we demonstrate the influence of out-of-plane spin torque on magnetization switching and susceptibility in a magnetic multilayer system. The variation of spin accumulation and local magnetization with respect to time are studied in the magnetization reversal induced by spin torque. We also research the susceptibility subject to a microwave magnetic field, which is compared with the results obtained without out-of-plane torque.  相似文献   

17.
The effect of Ba(La)TiO3 doping on the structure and magnetotransport properties of La2/3Sr1/3MnO3(LSMO)/xBa(La)TiO3 (x=0.0, 1.0, 5.0 mol%) have been investigated. The X-ray diffraction patterns and microstructural analysis show that BaTiO3 and LSMO phases exist independently in BaTiO3-doped composites. The metal-insulator transition temperature (TMI) decreases whereas the maximum resistivity increases very quickly by the increase of BaTiO3 doping level. The partial substitution of Ba by La(0.35 mol%) results in a decrease in resistivity of LSMO/xBa(La)TiO3 composites. Magnetoresistance of BaTiO3-doped composites decreases monotonously in the temperature range 200-400 K in a magnetic field of 5 T, which is completely different from that of LSMO compound. The value of MR decreases at low field (H<1 T) and increases at high fields (H>1 T) with increasing the BaTiO3 doping level at low temperatures below 280 K. These investigations reveal that the magnetotransport properties of LSMO/xBa(La)TiO3 composites are dominated by spin-dependent scattering and tunneling effect at the LSMO/BaTiO3/LSMO magnetic tunnel junction.  相似文献   

18.
(Ga1−xMnx)N thin films grown on GaN buffer layers by using molecular beam epitaxy were investigated with the goal of producing diluted magnetic semiconductors (DMSs) with band-edge exciton transitions for applications in optomagnetic devices. The magnetization curve as a function of the magnetic field at 5 K indicated that ferromagnetism existed in the (Ga1−xMnx)N thin films, and the magnetization curve as a function of the temperature showed that the ferromagnetic transition temperature of the (Ga1−xMnx)N thin film was above room temperature. Photoluminescence and photoluminescence excitation spectra showed that band-edge exciton transitions in (Ga1−xMnx)N thin films appeared. These results indicate that the (Ga1−xMnx)N DMSs with a magnetic single phase hold promise for potential applications in spin optoelectronic devices in the blue region of the spectrum.  相似文献   

19.
Transparent pure and Cu-doped (2.5, 5 and 10 at.%) anatase TiO2 thin films were grown by pulsed laser deposition technique on LaAlO3 substrates. The samples were structurally characterized by X-ray absorption spectroscopy and X-ray diffraction. The magnetic properties were measured using a SQUID. All films have a FM-like behaviour. In the case of the Cu-doped samples, the magnetic cycles are almost independent of the Cu concentration. Cu atoms are forming CuO and/or substituting Ti in TiO2. The thermal treatment in air promotes the CuO segregation. Since CuO is antiferromagnetic, the magnetic signals present in the films could be assigned to Cu substitutionally replacing cations in TiO2.  相似文献   

20.
    
Magnetoresistive random access memory (MRAM) is regarded as one of the leading candidates for universal memory [1] that will be commercialized in the foreseeable future. The figure of merits for MRAM technology includes non‐volatility, high speed, high density, radiation hardness, and unlimited endurance. Very promising R & D results have been announced wordlwide. For a high density MRAM as a standalone memory, uniform resistance and switching control for sub‐micron and deep sub‐micron devices must be guaranteed. To achieve this goal, several material and device issues related with MRAM core cell should be resolved. Resistance (R) as well as magnetoresistance (MR) are limited by the uniformity of barrier thickness induced by bottom electrode. Switching issues appear controllable with a choice of appropriate shape and fine patterning process. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

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