Pr2(Fe0.8Co0.2)14B磁结构的中子衍射研究

本文报道用中子衍射测定的含硼稀土过渡族金属间化合物Pr₂(Fe_0.8Co_0.2)₁₄B的晶体结构与磁结构。将中子三轴谱仪用作二轴粉末衍射仪,在室温测该化合物粉末样品的中子衍射强度,用轮廓精化法弥合衍射数据。该化合物属Nd₂Fe₁₄B类四方结构,α=8.8110?,c=12.2307?。设Pr,Fe和Co原子磁矩间为铁磁耦合,同一晶位的Fe,Co原子磁矩相等,存在沿c轴的易磁化 关键词：     

Magnetic properties of melt-spun Sm2+Y(Co0.8Fe0.1Mn0.1)17BX alloys

Melt-spun ribbons with composition Sm_2+Y(Co_0.8Fe_0.1Mn_0.1)₁₇B_X (X=0–1.0 and Y=0–0.2) were fabricated with a wheel speed of 50 m/s, followed by annealing in the temperature range of 500–800°C for 2.5–60 min. Our results show that all the ribbons annealed up to 800°C are composed of a TbCu₇-type phase as the main phase. The highest coercivity of 8.7 kOe is obtained in a Sm-rich sample with composition Sm_2.2(Co_0.8Fe_0.1Mn_0.1)₁₇ annealed at 750°C for 5 min. It is found that these magnets show a very promising high-temperature performance – much better than those of typical sintered 2 : 17 magnets.     

Mössbauer spectroscopy studies of spin reorientations in amorphous and crystalline (Co0.2Fe0.8)72.5Si12.5B15 glass coated micro-wires

Thermo-gravimetric, differential scanning calorimetry and comprehensive ⁵⁷Fe Mössbauer spectroscopy studies of amorphous and crystalline ferromagnetic glass coated (Co_0.2Fe_0.8)_72.5Si_12.5B₁₅ micro-wires have been recorded. The Curie temperature of the amorphous phase is T_C(amorp) ∼730 K. The analysis of the Mössbauer spectra reveals that below 623 K the easy axis of the magnetization is axial-along the wires, and that a tangential or/and radial orientation occurs at higher temperatures. At 770 K, in the first 4 hours the Mössbauer spectrum exhibits a pure paramagnetic doublet. Crystallization and decomposition to predominantly α-Fe(Si) and Fe₂B occurs either by raising the temperature above 835 K or isothermally in time at lower temperatures. Annealing for a day at 770 K, leads to crystallization. In the crystalline material the magnetic moments have a complete random orientation. After cooling back to ambient temperature, both α-Fe(Si) and Fe₂B in the glass coated wire show pure axial magnetic orientation like in the original amorphous state. The observed spin reorientations are associated with changes in the stress induced by the glass coating.     

Dy(Fe0.8Al0.2)2单晶体的宏观量子效应

测量了Dy(Fe_0.8Al_0.2)₂单晶体在[100],[110]和[111]方向上的退磁曲线、内禀矫顽力和磁黏滞性系数随温度的变化.认为退磁曲线出现台阶和大跳跃、内禀矫顽力随温度变化存在峰值、磁黏滞性系数与温度无关等都是畴壁隧穿能垒的宏观量子效应的反映.实验上得出由经典热激活到量子隧穿的交界温度约为5.5K. 关键词：     

Electrical resistivity of the pseudo-binary compound Ce(Fe0.8Al0.2)2

Electrical resistivity measurements on the alloy Ce(Fe_0.8Al_0.2)₂ as a function of temperature in the range of 1.5 to 300 K shows that the long range magnetic order of the CeFe₂ is destroyed and that the spin glass phase appears with a negative coefficient of T^3/2. The high residual resistivity is also discussed.     

EPR and optical properties of KYb(WO4)2 and KTb0.2Yb0.8(WO4)2 single crystals

Well oriented KYb(WO₄)₂ and KTb_0.2Yb_0.8(WO₄)₂ single crystals have been investigated for their magnetic and optical properties using the Raman and EPR techniques. The registered EPR signal is dominated by three lines ascribed to ytterbium ions: one main and two satellites. Tb ions, although non-paramagnetic, distinctly modify magnetic properties of the KYb(WO₄)₂ single crystal. Basic parameters of the spin Hamiltonian, including Zeeman and hyperfine terms (g and A matrices) as well the spatial orientation between principal and crystallographic axes systems were determined for both crystals.     

Heat capacity of the Nb3Al0.8Ge0.2 compounds

Heat capacity of the Nb₃Al_0.8Ge_0.2 samples have been measured in the temperature range 14–25K. It has been shown that the electron part of the heat capacity (γ) and the Debye temperature undergo only a small change after thermal treatment leading to significant increase of superconducting T_c. Such an increase of the band density of states N(E_F)_band may be caused by appropriate changes of phonon spectrum. The character of these changes is determined, to a great extent, by localization of the d-electrons in the niobium chains.     

(Ni0.8Zn0.2Fe2O4)epoxy-PZT双层膜中的磁电效应

讨论了Ni_0.8Zn_0.2Fe₂O₄ (NZFO)与锆钛酸铅(PZT)的双层膜结构样品的磁电(ME)效应.NZFO粉料由溶胶-凝胶法制成，再经900℃热压，并高温烧结.在该双层膜中测量到了很强的磁电相互作用.发现横向的磁电效应比纵向效应大一个数量级，并且随NZFO烧结温度的提高而增加.当烧结温度从950℃上升到1380℃时，横向ME电压系数(α_E)的最大值变化范围为25.6 mV Am^-2≤α_E≤199.6 mV Am^-2.理论分析显示NZFO-PZT双层膜样品中ME效应源于NZFO与PZT之间相对良好的磁电耦合. 关键词： 镍铁氧体 PZT 热压法 ME效应     

Magnetization process of Hf0.8Ta0.2Fe2 in strong pulsed magnetic fields

The magnetization process of an itinerant-electron magnet Hf_0.8Ta_0.2Fe₂ has been measured in pulsed magnetic fields up to 300 kOe at 4–330 K. The magnetic phase boundary in the high-field region has been determined and the temperature dependence of the high-field susceptibility in the ferromagnetic or saturated paramagnetic state is reported.     

铁基超导体Li0.8Fe0.2ODFeSe的红外光谱研究

测量和研究了铁基超导体Li_0.8Fe_0.2ODFeSe单晶的红外光学响应,发现室温下光电导率谱不存在Drude分量,载流子具有非相干输运行为.随着温度降低,Drude分量形成并不断变窄,同时在相应的反射率谱上出现清晰的等离子体边,表明散射率急剧降低.在最低温度,观察到超导能隙形成导致的光谱变化,光电导率谱在160 cm^-1以下受到显著压制.对比FeSe单晶的光谱数据,发现整体的光电导率谱型很相似,但自由载流子的谱重更低,揭示出样品具有更低的载流子浓度.另外还观察到温度变化诱导的谱重由低频向高频区域转移的现象,表明其存在强关联效应.     

Coil-less fluxgate effect in (Co0.94Fe0.06)72.5Si12.5B15 amorphous wires

In this study, the coil-less fluxgate properties of the as-cast and annealed amorphous wires with the composition (Co_0.94Fe_0.06)_72.5Si_12.5B₁₅ were investigated. As its name implies, a coil-less fluxgate is a new type of magnetic-field sensor without a coil. When the wire is periodically saturated in a magnetic field in the circumferential direction with a 30 kHz, 62 mA driving current under a 16.5π rad/m torsional strain, there is a linear variation in the second harmonic of the voltage from the wire ends as a function of the applied external DC magnetic field along the length of the wire.Current-stress annealing of each sample improved the sensitivity of the coil-less fluxgate sensor. This is the first time that it has been shown that a linear change in the output of the coil-less fluxgate sensor can be obtained using torsion annealed wire without the necessity of twisting the wire during measurement. We showed that the linear operating range of the sensor can be increased by increasing the demagnetization factor in the sensing direction, so that the coil-less fluxgate sensor can be miniaturised just by reducing the wire length.     

合成反铁磁Ni81Fe19/Co90Fe10/Ru/Co90Fe10/Ni81Fe19的研究

采用直流磁控溅射方法制备了一系列的合成反铁磁及以其为自由层的自旋阀.研究发现,在Ni₈₁Fe₁₉与Ru层之间插入适当厚度的Co₉₀Fe₁₀层后,可有效地提高合成反铁磁两磁性层间的反铁磁耦合强度,得到具有饱和场H_s更高、饱和磁化强度M_s更低、热稳定性更好的合成反铁磁.另外,以这种合成反铁磁作自旋阀的自由层时,可有效提高自旋阀的稳定性. 关键词： 合成反铁磁 退火 自旋阀     

(La0.2Nd0.8)0.67Pb0.33MnO3的Preisach分析

测量了居里点为TC=220K的钙钛矿(La0.2Nd0.8)0.67Pb0.33MnO3 (LNPMO)在外场为ha=3978.87A/m ，2K相似文献   

Electrical properties of amorphous (Co45Fe45Zr10)x(Al2O3)1?x nanocomposites

The electrical properties of (Co₄₅Fe₄₅Zr₁₀)_x(Al₂O₃)_1−x granular nanocomposites have been studied. The concentration dependences of electrical resistivity are S-shaped (in accordance with the percolation theory of conduction) with a threshold at a metallic component concentration of ∼41 at. %. An analysis of the temperature behavior carried out in the range 300–973 K revealed that structural relaxation and crystallization of the amorphous phase are accompanied by a decrease in the electrical resistivity of the composites above the percolation threshold and by its increase below the percolation threshold. For metallic phase concentrations x<41 at. %, variable range hopping conduction over localized states near the Fermi level was found to be dominant at low temperatures (77–180 K). A further increase in temperature brings about a crossover of the conduction mechanism from Mott’s law ln(σ) ∝ (1/T)^1/4 to ln(σ) ∝ (1/T)^1/2. A model of inelastic resonance tunneling over a chain of localized states of the dielectric matrix was used to find the average number of localized states involved in the charge transport between metallic grains. __________ Translated from Fizika Tverdogo Tela, Vol. 46, No. 11, 2004, pp. 2076–2082. Original Russian Text Copyright ? 2004 by Kalinin, Remizov, Sitnikov.     

快淬(Er1-xSmx)2Fe17Cy化合物的结构与磁性

用快速急冷方法制备了(Er_1-xSm_x)₂Fe₁₇C_y(x≤0.8,1.5≤y≤2.5)化合物,它们具有菱方Th₂Zn₁₇型结构,并且在高温是稳定的。与相应的不含C的(Er_1-xSm_x)₂Fe₁₇化合物比较,当C含量y=2.5时,引起单胞体积增加～6.3％,居里温度增     

Symmetric logarithmic heat capacity anomaly of the layered manganese compound: Mn(NH3)2Ni(CN)42C12H10

The magnetic susceptibility and the heat capacity of a layered manganese compound Mn(NH₃)₂Ni(CN)₄2C₁₂H₁₀ have been measured down to the antiferromagnetic ordered state. A similar symmetric logarithmic singularity in the heat capacity is found for the isomorphic nickel compound Ni(NH₃)₂Ni(CN)₄2C₁₂H₁₀ has been observed at T_N = 0.172 K.     

Giant magnetoimpedance in amorphous (Co0.93Fe0.7)63Ni10Si11B16 glass-coated microwire

Giant magnetoimpedance (GMI) effect has been measured in a glass-coated amorphous (Co_0.93Fe_0.7)₆₃Ni₁₀Si₁₁B₁₆ microwire as a function of DC magnetic field and up to the frequency of 11 MHz. The sample shows single peak GMI characteristics within the whole range of frequency. The domain structure of the above sample has been changed by applying tensile stresses up to 603 MPa and current annealing with a DC current of 50 mA for various time durations, and the corresponding effect on GMI has been studied in detail. A maximum change of 8.85% in MI of the as-quenched sample has been observed around a frequency of 5.05 MHz. Application of an external tensile stress reduces the GMI value by increasing the inner core domain, whereas heat treatment of the sample enhances the same. The square-shaped magnetic hysteresis loop of the as-quenched sample helps us understanding the MI results.     

Magnetization and demagnetization behaviours of melt-spun Pr12Fe82B6 and Pr8Fe87B5 ribbons

Nanocrystalline Pr_{12}Fe_{82}B_6 and nanocomposite Pr_8Fe_{87}B_5 ribbons have been prepared using a melt spinning technique. Recoil loops have been measured at 20, 200 and 300K. Demagnetization curves are analysed by dividing it into reversible and irreversible portions. High recoil loop susceptibility at low applied field and large reversible change in the demagnetization curve have been found in Pr_8Fe_{87}B_5 ribbons, showing that the reversible behaviours in nanocomposite permanent magnets originate primarily from the magnetically soft phase. The hysteresis in recoil loops found in Pr_8Fe_{87}B_5 ribbons originates from the soft phase α-Fe that suffers a stress.     

The effect of Ru doping on the alkali-doped manganite Pr0.8Na0.2MnO3

Polycrystalline manganites Pr_0.8Na_0.2MnO₃ doped by ruthenium (0.0≤x_Ru≤0.2) were prepared by the sol-gel process. The magnetic field induced metamagnetism was observed to occur with a large resistivity drop at 3 K for x_Ru≤0.02 samples, which can be sorted into the kind of CMR phenomenon. It was found that the 0.01 Ru doping increased T_C and decreased the metamagnetic critical field than that of the undoped sample. The doped manganites show a quick increase in their magnetic moments as x_Ru increases from 0.01 to 0.04, but the larger fraction of Ru doping (0.04≤x_Ru≤0.2) reduces their M and T_C. All the five doped samples have larger magnetic moments than that of the host sample. Ru doping of x_Ru>0.01 results in a rapid disappearance for the observation of long range spin and charge ordering in the samples’ M-T curves, which is characteristic of the undoped sample. It was found that larger low-temperature MR favored decrease in the metamagnetic critical field. Finally, the phase diagram of Ru doping vs. transition temperatures is presented to summarize the experiments.     

Magnetooptical properties and FMR in granular nanocomposites (Co84Nb14Ta2) x (SiO2)100? x

For nanodimensional magnetically inhomogeneous amorphous granular films of the system (Co₈₄Nb₁₄Ta₂) _x (SiO₂)_100−x , 30≤x≤60 at.% the concentration dependences of the magnetooptical Kerr effect (MOKE) spectra and FMR have been investigated. The observed changes in the MOKE and FMR spectra are associated with transformations of microstructure and topology of the nanocomposites. For the compositions within the percolation region the transversal Kerr effect increases by an order of magnitude.