不同晶粒尺寸的(La0.47Gd0.2)Sr0.33MnO3纳米颗粒磁性能

采用非晶态多核配合的方法制备了(La0.47Gd0.2)Sr0.33MnO3纳米颗粒,用XRD、HRTEM和MPMS等手段对纳米颗粒的微观结构和磁性能进行研究。XRD和SAD分析表明,所有的样品都具有单相钙钛矿结构;TEM分析表明, 经过600,800和1000 ℃烧结10 h后的样品颗粒尺寸分别为40~50 nm,90~100 nm和140~150 nm。样品的磁学性能结果表明：(La0.47Gd0.2)Sr0.33MnO3纳米颗粒的居里温度TC (298 K)基本上不随颗粒尺寸的变化而变化,而相对磁制冷能力取决于颗粒尺寸;颗粒尺寸为90~100 nm的(La0.47Gd0.2)Sr0.33MnO3纳米颗粒的相对磁制冷能力最大,可以作为室温下使用的磁制冷工质侯选材料。     

La_（0.85）K_（0.15）MnO_3多晶纳米颗粒磁制冷材料的制备

采用非晶态多核配合的方法在800℃制备出La0.85K0.15MnO3纳米颗粒,用XRD、HRTEM和PPMS等手段对纳米颗粒的微观结构和磁性能进行研究。XRD和ED分析表明,所有样品都具有单相钙钛矿结构;样品的M-T曲线研究结果表明,La0.85K0.15MnO3纳米颗粒的居里温度TC为242.65 K。     

稀土空位锰氧化物(La(1-x-y)Yy)2/3Ca1/3MnO3的磁热效应

采用固相反应法制备La(1.x)2/3Ca1/3MnO3(x=0.0,0.04)和(La0.7Y0.3)2/3Ca1/3MnO3系列样品,测量不同温度下的磁化强度-磁场曲线,计算样品的磁熵变,研究La空位掺杂和Y3 离子掺杂对磁热效应的影响.结果表明,La空位掺杂(x=0.04)的样品在居里温度附近磁熵变最大值为6.22 J/(kg.K),这比La2/3Ca1/3MnO3磁熵变最大值(6.26 J/(kg.K))稍有降低;而Y3 离子掺杂的样品在温度60 K时和磁场强度2 T下,其磁熵变最大值为0.568 J/(kg.K),并且磁熵变随温度变化有继续增大的趋势.这表明(La0.7Y0.3)2/3Ca1/3MnO3可以作为一定温区的磁致冷材料.     

Low-field magnetoresistance of (1-x)La_(0.6)Dy_(0.1)Sr_(0.3)MnO_3/0.5x (Sb_2O_3) composite system under different sintering temperatures of matrix

A series of (1-x)La0.6Dy0.1Sr0.3MnO3/0.5x(Sb2O3)(x=0.15) samples were prepared by the solid-state reaction method, and the influence of sintering temperature of the matrix on low-field magnetoresistance of (1-x)La0.6Dy0.1Sr0.3MnO3/0.5x (Sb2O3) was studied through the measurements of X-ray diffraction (XRD) patterns, scanning electron microscope (SEM) image, resistivity-temperature (ρ-T) curves, and magnetoresistance-temperature (MR-T) curves. The results indicate that for the samples with low sintering temp...     

油酸对化学共沉淀法制备La0.7（Ca0．53Sr0．47）0.3MnO3多晶的电阻温度系数的影响

研究了化学共沉淀法制备La0.7(Ca0.53Sr0.47)0.3MnO3多晶过程中添加油酸作分散剂的工艺,用DTG/TA、XRD和R-T(电阻-温度)系统测试了所制样品的性能.结果表明:添加油酸,共沉淀法制备La0.7(Ca0.53Sr0.47)0.3MnO3多晶比不添加的烧结温度低,也比同相反应法低.油酸的用量为0.1～O.2L/mol能明显提高La0.7(Ca0.53Sr0.47)0.3MnO3的电阻一温度转变点和电阻温度系数.     

La0.67Sr0.33Co1-xFexO3体系的输运行为

研究了Co位Fe掺杂对La0.67Sr0.33Co1-xFexO3体系的电输运性质和巨磁效应的影响.结果表明:电阻率在低掺杂(x≤0.1)时显示金属性输运行为,而在高掺杂(x=0.2,0.3)时则显示半导体行为.而且,Fe掺杂削弱了Tc处的MR峰值,但增加了低温下T≤Tc的MR值.La0.67Sr0.33Co1-xFexO3体系的磁电阻的起源可由外加磁场导致的自旋态转变来解释.     

La0.77-xCa0.2SrxMnO3纳米颗粒的磁热效应

用溶胶-凝胶法制备了La0.77-xCa0.2SrxMnO3钙钛矿材料,实验结果表明掺入少量Sr可显著调节样品的居里温度Tc至室温(由236 K提高至300 K),同时样品保持了较大的磁熵变.在1 T外场下,x=0.06的样品最大磁熵变2.32 J·kg-1K-1,Tc为271 K.该系列样品低磁场下在室温附近具有较大的磁熵变,可作为室温磁制冷材料.     

钙钛矿型锰氧化物La0.8Sr0.2MnO3的高频性能

采用溶胶-凝胶法制得La0.8Sr0.2MnO3氧化物多晶样品。通过XRD、SEM对样品的微观结构进行了分析,结果表明:所得样品为钙钛矿结构,样品的颗粒大小比较均匀,平均粒度约100nm。利用阻抗分析仪对样品的介电常数和磁导率的频谱(10MHz～1GHz和1MHz～1GHz)进行了研究。研究表明,在整个测试频率范围内,La0.8Sr0.2MnO3的介电常数实部和虚部随频率的升高而降低。La0.8Sr0.2MnO3的复磁导率的频谱谱线为典型的弛豫型谱线,磁导率实部在1MHz时为6.2,共振频率fr为50MHz,共振时虚部峰值为2.8;磁谱测试表明材料的弛豫损耗峰出现在频率f≤300MHz的频率范围内,在此频率区域引起损耗的机制主要是畴壁共振。     

La0.7Sr0.3MnO3和ZnO异质结的量子铁磁自旋特性

采用脉冲激光沉积方法制备La0.7Sr0.3MnO3/ZnO异质结,并对其量子铁磁自旋行为进行研究。发现掺杂浓度可有效调整长程的电子自旋和轨道的相互作用,以及短程小极化子的相互作用程度。LSMO/ZnO异质结构可对能带进行有效剪裁。XRD结果表明,所制样品具有良好的晶格外延特性。伏安特性和阻温曲线显示异质结具有半金属光导特性。在激光光场和磁场下测试La0.7Sr0.3MnO3/ZnO异质结量子铁磁自旋磁阻及光阻。结果发现,样品x=0.3在Tp=250K发生金属绝缘体相变而呈现半金属特性,在Tc=175K温度发生顺磁到反铁磁相变。连续激光下低于峰值温度220K和脉冲激光下低于175K区域激光光场导致光致退磁,光阻增大,在大于峰值温度Tp的高温区出现光阻降低。研究表明,在光场下La0.7Sr0.3MnO3/ZnO异质结特性受界面电子自旋取向和载流子浓度调控,态密度以及自旋轨道作用会导致光致阻抗变化,这些影响与LSMO/ZnO异质结的极化和界面应力所产生的界面态缺陷结构有关。     

Na^＋掺杂对钙钛矿La0．7Sr0．3-xNaxMnO3的结构及磁熵变的影响

采用溶胶-凝胶法制备了钙钛矿La0.7Sr0.3-xNa xMnO3(0.05≤x≤0.3)系列样品.结果表明:由于Na+离子半径(0.102 nm)小于Sr2+离子半径(0.127 nm),导致La0.7Sr0.3-xNaxMnO3(0.05≤x≤0.3)样品的结构随着Na+离子掺杂量的增加由正交向单斜转变.样品的晶胞参数a随x的增大而增大,而c随x的增大而减小,c/a随x的增加而减小;样品的形貌呈现不规则的颗粒状,中间还夹杂着棒状物;随着Mn4+与Mn3+摩尔比的增加,A位的平均离子半径减小及A位离子失配效应减小的共同影响下,当x≤0.2时,居里温度随着Na+离子掺杂量的增加而增加;当x＞0.2时,居里温度随着Na+离子掺杂量的增加而下降;由于Na+离子掺杂引起的容差因子的减小,晶格收缩、铁磁耦合变小,导致居里温度附近的最大磁熵变随x增加而减小.     

Structural, magnetic and magnetocaloric effect in double perovskite Ba2CrMo1−xWxO6

Magnetic refrigeration, an emerging new technology for cooling and gas liquefaction, needs magnetic materials with specific thermomagnetic behavior. Depending on the thermodynamic cycle selected, the isothermal magnetic entropy change or the adiabatic temperature change upon field application needs to be a preselected function of temperature. In double perovskite Ba₂CrMo_1−xW_xO₆ (x = 0, 0.2 and 0.5) prepared by the sol–gel method, the experimental results show the observation of a large magnetocaloric effect (MCE) near the Curie temperature T_C which decreases with the increasing of the substitution of Mo by W. The maximum of the magnetic entropy change peaks at the magnetic ordering temperature T_C, and a large magnetic entropy change (|ΔS_M| ≈ 1.6 J kg⁻¹ K⁻¹) is obtained at 285 K in the sample Ba₂CrMo_0.5W_0.5O₆ under an applied magnetic field of 10 kOe.     

LaFe11.9-xCoxSi1.1B0.2(x=0.7,0.8,0.9)合金的磁热效应

使用电弧熔炼法制备了LaFe11.9-xCoxSi1.1B0.2(x=0.7,0.8,0.9)系列合金.XRD分析表明该系列合金除微量的α-Fe相外,均由NaZn13型立方结构单相组成.晶格常数随着Co含量的增加而增大,分别为1.1487,1.1496,1.1498nm;磁性测量表明该系列合金的Curie温度在室温附近,并且也随着Co含量的增加而分别增加到270,290,300 K.在外场变化△B=1.5 T时,该系列合金的最大磁熵变均为金属Gd的2倍左右,相对制冷能力与金属Gd基本相同.     

磁一级相变La(Fe,Si)13基化合物的研究进展

对NaZn13型La(Fe,Si)13化合物在磁性、相变特性及磁熵变规律和制备方法等方面的研究进展进行总结和论述.低Si含量的La(Fe,Si)13化合物具有良好的软磁特性,表现出特殊的磁相变特征:在居里温度处的热诱导一级磁性转变和高于居里温度时的磁场诱导巡游电子变磁性转变,并伴随着巨大的磁熵变和磁致伸缩.随Si含量增高,化合物的这种特殊磁相变特征逐渐减弱,呈现二级相变特征.总结了元素替代和添加对La(Fe,Si)13化合物性能的影响,一定的合金化可以改变居里温度并保持巨大的磁熵变,这对于近室温磁致冷有着重要意义.快速凝固技术的应用解决了化合物合成困难的问题,降低了材料的制造成本,使得NaZn13型La(Fe,Si)13化合物成为最有应用前景的近室温磁致冷工质之一.本文还探讨了这种化合物用做磁致伸缩材料的可能性.     

Ni46Mn35Ga19单晶大的磁熵变和磁控形状记忆效应

采用多种测量手段,对制备出的转变温度在室温以上的Ni46Mn35Ga19单晶的物性进行表征。电阻和交流磁化率结果表明,该材料的磁转变和马氏体相变是同时发生的。定温磁化强度测量得出材料磁熵变的增长速率高达9.0J/kg·K·T,在1274kA/m(1.6T)的磁场下,磁熵变达13.8J/kg·K。此外,应变测量表明,伴随该磁熵变,材料展现出应变量分别高达–0.89%和–1.90%的自发和磁控双向形状记忆效应。     

Magnetic entropy change in polycrystalline La1−xKxMnO3 perovskites

Polycrystalline samples of potassium doped lanthanum manganites having nanometric crystallite size have been synthesized by pyrophoric method. The Curie temperature (T_C) of the prepared samples is found to be strongly dependent on K content and spans between 260 and 309 K. Close to T_C, large change in magnetic entropy has been observed in all the samples. The maximum magnetic entropy change observed for samples with different concentration of K, exhibits a linear dependence with the applied magnetic field. Adiabatic temperature change at T_C at 1 T also increases with K doping and attains a maximum of 2.1 K for La_0.85K_0.15MnO₃. Estimated relative cooling power of La_1−xK_xMnO₃ compounds is nearly one-third of pure Gd. In addition to the tuneability of T_C between 260 and 310 K, higher chemical stability, lower eddy current heating and inexpensive preparation technique; the magnetic entropy change in La_0.85K_0.15MnO₃ compound at 1 T magnetic field is found to be 3.00 J/kg K and is 89% to that known for the prototype magnetic refrigerant (pure Gd). Our result on magnetocaloric properties suggests that La_1−xK_xMnO₃ compounds are attractive as a possible refrigerant for near room temperature magnetic refrigeration.     

Enhanced magnetic refrigeration capacities in minutely Co doped Mn5-xCoxGe3 compounds

Mn₅Ge₃ is a ferromagnetic compound with a Curie temperature of 299 K that exhibits a large magnetocaloric effect near room temperature. Here, we have synthesized and characterized a series of Co doped Mn_5-xCo_xGe₃ samples, in an attempt to improve the magnetocaloric properties of the system. X-ray diffraction measurements revealed that all samples exhibit the Mn₅Si₃-type D8₈ hexagonal structure at room temperature with no significant change in the lattice parameters between samples, while scanning electron micrographs showed that all samples exhibit a single compositional phase. Magnetization measurements show a decrease in Curie temperature concurrent to increasing Co concentration. Although, the magnitude of the peak magnetic entropy change stays nearly constant across the series, increased Co substitution significantly enhances the refrigerant capacity of the materials. The largest magnetocaloric effects are observed in the Mn_4.85Co_0.15Ge₃ compound with a peak magnetic entropy change of 7.58 J/kg K and a peak refrigeration capacity of 380.32 J/kg for a magnetic field change of 50 kOe.     

Er2-xPrxFe17磁致冷合金在室温区的磁熵变

在氩保护气氛中用熔炼法制备了Er2-xPrxFe17系列合金，通过X射线衍射和SQUID磁强计研究了样品的结构和磁熵变。结果表明，Er2-xPrxFe17系列合金具有六方Th2Ni17型结构，通过成分微调使其居里温度处在室温附近，Er2-xPrxFe17合金有较大的磁熵变，且致冷温区较宽，是一类有很大应用潜力的室温磁致冷材料。     

The origin of the large magnetocaloric effect in RCo2 (R=Er, Ho and Dy)

The phase transitions of the RCo₂ (R=Er, Ho and Dy) compounds are of first-order type and a metamagnetic transition is observed above the Curie temperature. Owing to their large magnetic entropy change, the RCo₂ compounds are competitive candidates as the working substance for magnetic refrigeration. In this paper we discuss the origin of this large magnetic entropy change.     

Gd0.95Nb0.05合金磁热效应的研究

采用X射线衍射技术、直接磁热效应测量仪和VSM振动样品磁强计研究电弧熔铸和400℃,1h热处理后低纯Gd0.95Nb0.05合金的磁热效应。结果表明:适量Nb的加入不改变商业Gd的居里温度,但明显提高了商业Gd的磁热效应,最大绝热温变由3.1K增加到3.5K,1.5T磁场下最大磁熵变为3.99J/(kg·K);Gd0.95Nb0.05合金经过400℃,1h热处理后,居里温度提高了2K,最大绝热温变和最大磁熵变有不同程度的增加。与高纯Gd相比,商业原料制备的Gd0.95Nb0.05合金成本低廉,是一种非常实用的磁制冷工质材料。     

Gd-Tb-Nd系室温磁致冷材料研究

对适用于室温区磁致冷的Gd Tb Nd系合金进行了研究。样品用Ar气保护的高频磁浮炉熔炼 ,用振动样品磁强计测量了不同温度下的磁化曲线。根据整理的磁热曲线计算出材料的磁熵改变值。结果表明 :GdxTbyNd( 10 0 -x - y) 系磁致冷材料的居里温度在室温附近 ,Tb和Nd含量的增加使居里温度降低 ;Nd含量较小时Gd Tb Nd系具有较大的磁熵改变值 ;少量Nd的加入可显著改变居里温度 ,是十分有效的制冷温区调节剂。因此 ,采用不同成分的Gd Tb Nd系材料的组合 ,可望实现在低磁场下室温附近较大温度范围的磁制冷热循环。