自旋玻璃的重入行为及Co_xZn(1-x)(Fe_yCr(1-y))_2O_4尖晶石系统的磁相图

本文研究了Co_xZn-(1-x)(Pe_yCr(1-x)_2O_4尖晶石系统的磁性,测量了不同成份样品的低频弱场交流磁化率与低场直流磁化强度的温度关系。根据实验结果,给出了该系统可能的磁相图。发现在该系统中相当宽的成份范围内,都存在自旋玻璃的重入现象。同时发现,自旋玻璃的重入温度随磁性离子浓度增加而增加。这些行为是磁性离子浓度含量较高和多种磁性离子共存系统的共同特性。还讨论了自旋玻璃重入行为的机制。认为该尖晶石系统中的重入自旋玻璃态,是由亚铁磁长程序解体而形成的大量亚铁磁微畴或自旋团与自旋玻璃共存的状态。     

重入自旋玻璃尖晶石系统CoxZn1-x(FeyCr1-y)2O4中的微波磁共振

研究了具有重入自旋玻璃转变的尖晶石系统Co_xZn_1-x(Fe_yCr_1-y)₂O₄(0.4≤x≤0.8,y=O.5,0.8)中的微波磁共振,获得了共振线型、共振线宽、共振场、g因子、积累强度等共振参数与温度的依赖关系,并研究了磁性离子Co²⁺的浓度对共振线宽的影响。采用自旋成团效应及局域混乱场模型讨论了这些实验现象的机制,认为在一定条件下自旋团的形成、发展 关键词：     

Zn1-xMnxSe的低温磁化率和自旋玻璃现象

用超导量子干涉器(SQUID)磁强计对稀释磁性半导体Zn_1-xMn_xSe(0.1≤x≤0.50)的低温低场直流磁化率作了测量,测量温度从4.2K到30K,测量磁场为15Oe。当x≥0.30时,从磁化率-温度曲线的浑圆峰值,观察到了自旋玻璃的转变。自旋玻璃的转变温度T_f,对x=0.30,0.40,0.50,分别为10.5K,16K,19.5K。给出了顺磁相和自旋玻璃相的相图。比较了Zn_1-xMn_xSe和Cd_1-xMn_xSe的自旋玻璃转变温度,发现对同样的Mn离子浓度,Zn_1-xMn_xSe的T_f高于Cd_1-xMn_xSe的T_f,用交换作用的理论作了讨论。 关键词：     

(Nd1－xGdx)3Fe27.31Ti1.69化合物的结构和磁性

通过X射线衍射和磁性测量等手段研究了(Nd_1-xGd_x)₃Fe_27.31Ti_1.69(0≤x≤0.6)化合物的结构和磁性.X射线衍射测量结果表明Gd替代后并未改变Nd₃(Fe,Ti)₂₉化合物的晶体结构，但引起了晶胞体积收缩.随着Gd含量的增加，化合物的居里温度T_C和室温磁晶各向异性场B_a单调增加，而自旋重取向 关键词： 1-xGd_x)₃Fe_27.31Ti_1.69化合物')" href="#">(Nd_1-xGd_x)₃Fe_27.31Ti_1.69化合物 磁晶各向异性 自旋重取向 磁相图     

Eu2－xPbxRu2O7中的金属-绝缘体相变和自旋玻璃态行为

通过对Eu_2-xPb_xRu₂O₇(x=0.0, 0.2, 0.4, 0.6, 0.8, 1.0和1.8)系列样品的结构、电阻和磁化率的观测，结果发现，随着Pb替代浓度x值的增加，样品的电阻率逐渐减小，系统在x=0.8附近发生了金属-绝缘体(M-I)相变；Ru⁴⁺的局域磁矩及其自旋玻璃冻结温度T_G也随之降低. 在该体系中，Pb²⁺对Eu³⁺的部分替代使样品中载流子浓度增加，Pb的6p能带与Ru 4d电子的T_2g能带混合，能带得以拓宽，Ru 4d电子的巡游性增强，导致该体系物性的系列变化. 关键词： 自旋几何受挫 2-xPb_xRu₂O₇体系')" href="#">Eu_2-xPb_xRu₂O₇体系 金属-绝缘体相变 自旋玻璃态     

非晶态Fe90-xMnxZr10合金的磁性

本文报道用单辊急冷方法制备的非晶态合金Fe_90-xMn_xZr₁₀(x=0,4,6,10,15)的磁性,讨论了样品中每个原子的平均磁矩和居里温度T_c随Mn含量x的变化以及类自旋玻璃特性,给出了非晶态Fe_90-xMn_xZr₁₀合金的磁相图。观察到非晶态Fe₈₄Mn₆Zr₁₀合金晶化后的热磁曲线 关键词：     

镨离子掺杂对SrFe12O19结构和磁性的影响

通过机械球磨和后续热处理工艺,制备了镨离子掺杂的各向同性Pr_1-xSr_xFe₁₂O₁₉磁性粉末.研究了离子掺杂浓度和退火条件对样品结构和磁性的影响.结果表明,镨离子掺杂导致单相硬磁化合物的形成温度升高.成分的改变不会影响样品的居里温度,而退火温度的升高导致居里温度略有下降.一定含量的镨掺杂可适当增加样品的矫顽力,但导致磁化强度降低.不同成分样品的磁性受退火温度影响规律不同. 关键词：     

稀释磁性半导体Sn1-xMnxO2的室温铁磁性

采用固相反应法，制备了不同成分的稀释磁性半导体Sn_1-xMn_xO ₂(x=002，004，006)．利用x射线衍射和傅里叶变换红外光谱法证明 了锰均匀地掺杂到二氧化锡中．在室温下研究了掺锰二氧化锡基稀释半导体的磁性，发现它具有明显的铁磁性 ，同时对磁性的强弱与锰的含量和烧结温度的关系作了研究． 关键词： 稀释磁性半导体 掺杂 烧结 铁磁性 1-xMn_x O₂')" href="#">Sn_1-xMn_x O₂     

钙钛矿型稀土锰氧化物La2/3Ca1/3MnO3中Mn位的Ti替代效应

研究了钙钛矿型锰氧化物La_2/3Ca_1/3Mn_1-xTi_xO₃(0≤x≤0.3)的结构、磁性和输运性质.发现Ti替代Mn强烈地抑制了La_2/3Ca_1/3MnO₃的铁磁性和金属电导,并很大地提高了磁电阻值.在低掺杂情况下(x≤0.04),1%的Mn被Ti替代,居里温度T_C和金属-绝缘体转变温度T_p分别平均下降了31和26.5K.当x=0.06时,铁磁态过渡为团簇玻璃态,并在x=0.20时完全变为自旋玻璃态.指出由于Ti的掺入而引起的磁稀释作用以及局域晶格畸变是产生上述结果的主要原因. 关键词：     

非晶态快离子导体(AgI)x(Ag4P2O7)1-x的声学性质

用液氮骤冷方法制备了(AgI)_x(Ag₄P₂O₇)_1-x系列非晶态快离子导体。对AgI摩尔浓度x=0.50,0.60,0.67,0.75,0.80的样品,在77—300K温度范围及2,5,10,15MHz的频率上测量了纵波和横波的超声衰减和声速。发现在200—240K附近存在一个异常强的弛豫型超声吸收峰,随AgI含量的增加,该峰的位置向低温方向移动,且峰的高度增大。在实验的温度范围内,观察到纵波和 关键词：     

Cluster spin glass ordering in diluted spinel Zn0.5Co0.5FeCrO4

The disordered spinel system, Zn_0.5Co_0.5FeCrO₄ has been investigated using the low field magnetization and ac susceptibility measurements. From the present results it appears that this system orders into a cluster spin glass state with the magnetic moments of the ferrimagnetic clusters randomly frozen. Compared to the Ni and Co zinc ferrites with the same magnetic dilution, introduction of Cr into the B sites appears to increase the frustration and disorder dramatically. The predicted phase diagrams for the ordering in diluted magnetic spinels do not describe the magnetic behaviour of this system, presumably due to the disorder in the B sublattice in addition to the dilution in the A sublattice.     

低掺杂La1-xSrxMnO3结构相变对其电磁特性的影响

高温高压条件下，低掺杂的La_1-xSr_xMnO₃化合物发生从菱方相(R3c)到立方相的转变，该相变使其从低温时的绝缘态(极化子有序)转变为金属态.同时，随温度的降低，局域锰离子的自旋也从铁磁长程有序变成了只有短程序结构的自旋玻璃态.这种转变是由于相变引起的Mn—O—Mn键角及Mn—O键长的改变所引起. 关键词：     

Re-entrant superconductivity in a magnetically ordered superconductor: La1-xGdxRu2

We have measured the critical temperature (T_c) and the upper critical magnetic field (H_c2) of La_1-xGdxRu₂. At low concentrations of the magnetic impurity (Gd), the suppression of T_c follows the expected Abrikosov-Gorkov (A-G) pair breaking curve. However, for larger concentrations, strong deviations below A-G are observed. Samples in this region (4. ? × ? 5. at. %) exhibit two T_c's. La_1-xGd_xRu₂ is known to order magnetically, probably as a spin glass, and the magnetic ordering temperature (T_M) has been measured in the normal state. This T_M curve intersects the T_c curve in the concentration range where the T_c curve is re-entrant and we therefore attribute the re-entrant T_c behavior to the magnetic ordering of the Gd³⁺ ions.     

Magnetic properties of the mixed spinel Mg1+xMnxFe2-2xO4

The structural and magnetic properties of the mixed spinel Mg_1+xMn_xFe_2-2xO₄ system for 0.1<= x <= 0.9 have been studied by means of X-ray diffraction, magnetization, a.c. susceptibility and Mössbauer spectroscopy measurements. X-ray intensity calculations indicate that Mn⁴⁺ ions occupy only octahedral (B) sites replacing Fe³⁺ ions and the added Mg²⁺ ions substitute for A-site Fe³⁺ ions. All samples are magnetic at 12 K displaying Mössbauer spectra that have magnetic sextets coexisting with a central doublet that increases in population with increasing Mn concentration, indicating the presence of short range ordering (clustering). The Mössbauer intensity data show that Mn possesses a preference for the B-site of the spinel over the whole range of concentration. As expected, the hyperfine field and Curie temperature determined from a.c.susceptibility data decrease with increasing Mn content. Magnetization results indicate that on increasing dilution x, the collinear ferrimagnetic phase breaks down at x = 0.3 before reaching the ferrimagnetic percolation limit (x=0.6), as a result of the presence of competing exchange interactions, which is well supported by Mössbauer results. From all the above results, it is proposed that with increasing Mn content from x=0.6 to 0.9, the frustration and disorder increase in the system suppressing the ferrimagnetic ordering, and the system approaches to a cluster spin glass type of ordering at x=0.8 as reflected in the a.c.susceptibility and Mössbauer spectrum.     

MAGNETIC PROPERTIES AND CRYSTALLIZATION OF THE RAPIDLY QUENCHED (Fe1-xNdx) 81.5B18.5 ALLOYS

Magnetic properties and crystallization behaviors of amorphous (Fe_1-xNd_x) _81.5B_18.5 alloys were studied. The crystallization temperature is found to rise at first and then drop monotonically with x, having a maximum value of 976K at x=0.11 (9at% Nd). The (Fe_1-xNd_x) _81.5B_18.5 alloys prepared at a quenching rate of v_s = 6.6m /s are amorphous, and exhibit good glass formability. Both the coercive field H_c and energy product (BH)_max depend strongly on Nd concentration. Amorphous (Fe_1-xNd_x) _81.5B_18.5 alloys with higher Nd concentration have a high coercive field at low temperature, due to the large random uniaxial anisotropy of Nd. The room-temperature H_c and (BH)_max obtained on optimal annealing con-ditions show two maxima as a function of Nd concentration x. The highest room-temperature coercive field H_c =22 kOe within the Nd concentrations around x=0.368 and the maximum energy product(RH)_max= 13.3 MG·Oe at x =0.055 are observed. The hard magnetic properties of these crystallized samples are related to the presence of the bard magnetic Nd₂Fe₁₄B phase.     

Enhanced magnetization and ferrimagnetic behavior of normal spinel ZnFe2O4 thin film irradiated with femtosecond laser

We report on spatially selective change of magnetism from paramagnetic to ferrimagnetic-like behaviors in normal spinel ZnFe₂O₄ thin film under irradiation with 780 nm femtosecond laser pulses. The distribution of Zn²⁺ and Fe³⁺ ions in the irradiated region on the film surface becomes disordered because of local heating to high temperatures, and the metastable phase of ZnFe₂O₄ is frozen in by the rapid quenching after irradiation, resulting in the formation of the ferrimagnetic phase. The ferrimagnetic phase reverts to the paramagnetic state by annealing at 800°C. The present technique is useful for two-dimensional patterning of magnetic thin films.     

Er2(Fe1-xCox)15Ga2化合物的磁晶各向异性

通过X射线衍射和磁性测量等手段研究了Er₂(Fe_1-xCo_x)₁₅Ga₂化合物的结构与磁性，重点讨论了它们的磁晶各向异性.实验结果表明，Er₂(Fe_1-xCo_x)₁₅Ga₂化合物均为Th₂Ni₁₇型六角结构，晶格常数a,c和单胞体积V随Co含量的 关键词：     

Bi(Fe1-xMnx)O3的结构与磁性

使用快速烧结和溶胶-凝胶方法制备了Bi(Fe_1-xMnx)O₃的块材陶瓷,其x能够达到0.3,因而可以得到较细的粉末. 经X射线衍射谱和拉曼光谱研究发现其结构转变取决于锰的掺杂浓度. 当x=0.05和0.1时,Bi(Fe_1-xMnx)O₃的结构保持斜方六面体结构;当x=0.3时,Bi(Fe_1-xMnx)O₃的结构变化到正方六面体结构.在x=0.05和0.1时观测到弱铁磁性,但在x=0.3时观测到强顺磁性. 这显示了Bi(Fe_1-xMnx)O₃从反铁磁性到顺磁性的磁相变,同时也表明其结构从R3C变化到C222. 在30和140 K, x=0.05和0.1时,观察到Bi(Fe_1-xMnx)O₃的两个反常现象. 在30 K时,直流磁记忆和缓慢测量Bi(Fe_1-xMnx)O₃团族的反常现象与冷冻的旋转玻璃系统有关.