磁流体制备及性质研究

采用化学共沉淀法制备了纳米Fe3O4磁性颗粒,将其均匀分散在载液中获得磁流体.给出了表征所制备样品的宏观和微观特性图谱,探究了样品的磁热效应、法拉第效应和克尔效应,并制作了磁流体薄膜显示器.通过对磁流体样品的分析,获得其最佳的油酸钠包裹量为0.0216g/mL,样品颗粒小,稳定性高,磁热效应明显.研究发现磁流体薄膜的透射率随磁场变化明显,测量费尔德系数时必须考虑透射率的影响.磁流体样品存在异常克尔信号.     

Preparation of magnetite aqueous dispersion for magnetic fluid hyperthermia

An aqueous magnetic suspension was prepared by dispersing amphiphilic co-polymer-coated monodispersed magnetite nanoparticles synthesized through thermal decomposition of iron acetylacetonate (Fe(acac)₃) in a mixture of oleic acid and oleylamine. The average diameter of narrow-size-distributed magnetite nanoparticles varied between 5 and 12 nm depending on the experimental parameters such as reaction temperature, metal salt concentration and oleic acid/oleylamine ratio. Though the as-synthesized particles were coated with oleate and were dispersible in organic solvent, their surfaces were modified using amphiphilic co-polymers composed of poly(maleic anhydride-alt-1-octadecene) and polyethylene glycol-methyl ether and made dispersible in water. Infrared spectra of the sample indicated the existence of −COOH groups on the surface for further conjugation with biomolecules for targeted cancer therapy.     

Synthesis and properties of magnetic fluid based on iron nanoparticles prepared by a vapor-phase condensation process

Magnetic fluid containing metallic iron nanoparticles was successfully fabricated in this work. The iron nanoparticles were synthesized by chemical vapor condensation process and then dispersed in water-base solution (pH 11) with oleic acid as surfactant. More than 80% of iron nanoparticles were fully dispersed in the fluid and remained stable without any further oxidation over 200 h. Both the iron nanoparticles and the subsequent magnetic fluid exhibited typical ferromagnetic behavior.     

External influence on magnetic properties of Fe-based nanocrystalline alloys

Amorphous and nanocrystalline ribbons of NANOPERM, FINEMET and HITPERM were studied by Mössbauer spectroscopy (MS) after the influence of external factors: different annealing atmospheres, tensile stress and several kinds of corrosion. MS is a suitable tool for such studies because the spectral parameters are very sensitive to changes in the vicinity of the probe — ⁵⁷Fe nuclei. The most sensitive parameters were hyperfine magnetic field in crystalline component, average hyperfine field in amorphous component and direction of net magnetic moments. Influence of external factors modified also the structure of the alloys, i.e. new or modified phases were identified by MS phase analysis.     

The influence of defects on magnetic properties of fcc-Pu

The influence of vacancies and interstitial atoms on magnetism in Pu is considered in the framework of the density functional theory. The crystal structure relaxation arising due to various types of defects is calculated using the molecular dynamics method with a modified embedded atom model. The local density approximation with explicit inclusion of Coulomb and spin-orbit interactions is applied in matrix invariant form to describe correlation effects in Pu with these types of defects. The calculations show that both vacancies and interstitials give rise to local moments in the f-shell of Pu in good agreement with experimental data for aged Pu. Magnetism appears due to the destruction of a delicate balance between spin-orbit and exchange interactions.     

Rheological properties of water-based magnetic fluid and its emulsion

Field-induced rheological properties were studied for pure magnetic fluids (MFs) and 5% MF–cetyltrimethylammonium bromide (CTABr) emulsion for varying CTABr concentration (0–0.1 M) at different temperatures. The zero-field rheological study for 5% MF–CTABr emulsion shows maximum viscosity for 0.01 M CTABr concentrations. In-field viscosity results for 0.01 M CTABr–MF emulsion shows nearly 10 times more change in viscosity than the pure fluid, indicating the interaction between micelles and magnetic particles.     

An influence of pressure on magnetic properties of some amorphous alloys

Abstract

The paper presents the results of measurements of of magnetic properties of some Fe based amorphous alloys. The magnetization curves B(H) have been investigated within the range of pressure up to 2.5 GPa showing considerable changes with pressure. The reduction of spontaneous magnetization has been observed due to the pressure shift of Curie temperature. In some cases the total disappearence of ferromagnetism with increase of pressure has been observed at isothermal conditions.     

Synthesis and investigation of magnetic properties of Gd-substituted Mn–Zn ferrite nanoparticles as a potential low-TC agent for magnetic fluid hyperthermia

Gd-substituted Mn–Zn ferrite nanoparticles of different compositions were synthesized by chemical co-precipitation method. To study the reduction of the Curie temperature (T_C) for different samples, their magnetic properties in dependence from the composition and cationic distribution were investigated. An attempt to lower the T_C of superparamagnetic particles to the optimal temperature required in magnetic fluid hyperthermia (44–47 °C) was made.     

The structuralization phenomena in magnetic fluid composites and their influence on transmissivity of light

A magnetic field induced agglomeration of magnetic and μm-sized copper non-magnetic particles in magnetic fluid with several volume concentrations of magnetite and copper particles was studied by means of optical microscope equipped with video camera. Transmission of light through two crossed polarizers and thin magnetic fluid and magnetic fluid composites film as a function of magnetic field was investigated. The experimental data showed that the presence of copper particles influences the aggregation processes of magnetic particles in magnetic fluids and transmissivity of light. Dedicated to Dr. Anton Zentko on the occasion of his 60th birthday. This work was supported by the Slovak Academy of Sciences within the framework of Project GAV No. 4001.     

The influence of ball-milling on structural and magnetic properties of Co-based powders

The melt-spun Co- and Fe-based amorphous alloys have been investigated extensively for applications in magnetic devices, which require magnetically soft materials. Although these alloys exhibit excellent soft magnetic properties, their thin sheet shape, which is a consequence of the low glass forming ability, limits significantly their engineering applications. A powder metallurgy is thus an alternative way of producing bulk and, at the same time, soft magnetic materials, having desired shape. In our case, Co₅₆Fe₁₆Zr₈B₂₀ and Co_70.3Fe_4.7Si₁₀B₁₅ amorphous ribbons have been ball-milled for a short time and subsequently compacted (by hot pressing) into disc-shaped specimens with the aim to achieve samll values of resulting coercivity. This work is focused only on the first preparation step i.e. on structural and magnetic properties of ball-milled powders obtained by ball-milling of Co-based melt-spun ribbons at different conditions. Two different ways of milling were employed in order to obtain a powder form of the material: the ribbons were either continuously ball-milled for up to 12 hours or, after each half an hour of ball-milling, the vials were cooled in liquid nitrogen bath for half an hour. Mössbauer spectroscopy, X-ray diffraction and differential scanning calorimetry were employed to compare and to present the differences between these two different ways of milling.     

Synthesis and magnetic properties of Li-Mn-Zn spinel oxides

LiMn_2−XZn_XO₄ (X<0.5) compounds were prepared by sol-gel method. The specimens with a large substitution degree (X>0.2) led to symmetry reduction from Fdm to P2₁3 in the spinel oxide, while those with a small substitution degree (X<0.1) had Fdm cubic symmetry. The Zn²⁺-substitution led to the enhancement of the low-temperature magnetic susceptibility and a shift in the Weiss constant from negative to positive, indicating that the dominant exchange interaction changed from antiferromagnetic to ferromagnetic. For the compounds with X=0.5, the spontaneous magnetization was 4.48μ_B and the Curie temperature was approximately 21 K. The experimentally obtained magnetization value was close to the value calculated under the assumption that the spins of the Mn⁴⁺ ions were aligned in ferromagnetic form. In addition, the magnetic properties of Li-Mn-Zn spinel oxides were briefly discussed, and compared with those of Li-Mn-M (M=Ni, Mg) spinel oxides.     

Synthesis and magnetic properties of size-selected CoPt nanoparticles

CoPt nanoparticles are widely studied, in particular for their potentially very high magnetic anisotropy. However, their magnetic properties can differ from the bulk ones and they are expected to vary with the particle size. In this paper, we report the synthesis and characterization of well-defined CoPt nanoparticle samples produced in ultrahigh vacuum conditions following a physical route: the mass-selected low energy cluster beam deposition technique. This approach relies on an electrostatic deviation of ionized clusters which allows us to easily adjust the particle size, independently from the deposited equivalent thickness (i.e. the surface or volume particle density in a sample). Diluted samples made of CoPt particles, with different diameters, embedded in amorphous carbon are studied by transmission electron microscopy and superconducting interference device magnetometry, which gives access to the magnetic anisotropy energy distribution. We then compare the magnetic properties of two different particle sizes. The results are found to be consistent with an anisotropy constant (including its distribution) which does not evolve with the particle size in the range considered.     

Composition influence on the microstructures and magnetic properties of FePt thin films

The Fex Pt 100x (10nm) (x=31-51) thin films are fabricated on Si (100) substrates by using magnetron sputtering. The highly ordered L1 0 FePt phase is obtained after post-annealing at 700℃in Fe 47 Pt 53 thin film. The sample shows good perpendicular anisotropy with a square loop and a linear loop in the out-of-plane and the in-plane direction, respectively. The variations of the magnetic domains are investigated in the films when the content value of Fe changes from 31% to 51%.     

磁流体光栅的制作原理和磁性流体

介绍了磁流体光栅的制作原理、方法和磁性流体原理。     

The influence of magnetic heat treatment on morphology,structure, magnetic properties of Fe-Co-P alloy films

FeCoP nanocrystalline films were successfully electrodeposited on the Cu film coated silicon substrate in the bath containing Fe²⁺, Co²⁺, as well as different concentration H₂PO^? ions ranging from 0.001 mol/L to 0.01 mol/L. And then the samples experienced magnetic heat treatment with different heating rates. Effects of H₂PO^? concentration and magnetic heat treatment on morphological, structural, and magnetic properties of the films were investigated by scanning electron microscopy, X-ray diffraction, vibrating sample magnetometer, and vector network analyzer. The results suggest that the as-deposited films do not exhibit obvious in-plane uniaxial magnetic anisotropy, and interestingly after magnetic heat treatment at heating rate of 6?°C/min, the FeCoP films will possess better in-plane uniaxial magnetic anisotropy. It has been obtained that morphology and grain size play important roles in determining magnetic properties. The magnetic performance of FeCoP films with different phosphorus content can be improved by appropriate magnetic heat treatment.     

The influence of a magnetic field on the inelastic properties of LiF crystals

The effect of weak magnetic fields (0.1–0.8 T) on the internal friction and Young’s-modulus defect of LiF crystals is investigated over a range of relative strain amplitudes ɛ ₀ from 10⁻⁶ to 10⁻⁴ at frequencies of 40 and 80 kHz. Experiments with these fields show that the internal friction increases and the effective elastic modulus decreases, indicating an increase in the plasticity of the samples. Plots are obtained of the internal friction versus the magnitude of the magnetic field at various values of the strain amplitude ɛ ₀. Fiz. Tverd. Tela (St. Petersburg) 41, 1035–1040 (June 1999)