Destruction of charge ordering phase in La_（0.4）Ca_（0.6）MnO_3 induced by low Cr doping

Polycrystalline samples of La<0.4>Ca<,0.6>Mn<,1-x>Cr<,x>O<,3> (x = 0.00, 0.02, 0.04, 0.06) were prepared by the solid state reaction method. The influence of Cr<'3+> substitution for Mn<'3+> on the magnetic property and charge ordering phase of La<0.4>Ca<,0.6>MnO<,3> was studied through the measurements of X-ray diffraction (XRD), magnetization-temperature (M-T) curves and electron spin resonance (ESR) spectra. The experimental results indicate that the mother's body of La<,0.4>Ca<,0.6>MnO<,3> has very complicated magnetic structure, exhibits charge ordering phase at 258 K, and shows long-range strongly correlated charge ordering-antiferromagnetism (CO-AFM) phase from 175 to 50 K.Spin glass state appears when the tempereature decreases to about 41 K. When the Cr substitution amount is x = 0.06, the charge ordering phase of the mother's body is de- stroyed, because the Cr<'3+> substitution for Mn<'3+> destroys the spin order of CE-type antiferromagnetism, and thus leads to the melting of charge ordering. It is verified experimentally that the strong coupling between charge order and spin order exists in the charge order system of CE-type antiferromagnetism     

La1/3Sr2/3Mn1-xFexO3(x=0,0.05)中电荷有序现象的超声研究

系统研究了La1／3Sr2／3Mn1-xFexO3(x=0，0．05)单相多晶样品在20--300K温区内的电荷输运性质和超声特性，结果表明，La1／3Sr2／3MnO3样品在235K存在明显的电荷有序现象，但是极少量的Fe取代Mn就会有效地抑制电荷有序现象的发生，伴随电荷有序现象的发生声速出现极大的软化，其相对变化超过5％，这表明La1／3Sr2／3Mn1-xFexO3中存在剧烈的电-声子相互作用，分析指出该电-声子耦合主要起源于Jahn-Teller效应。     

X RAY DIFFRACTION STUDY OF THE THERMALLY INDUCED γ ε MARTENSITIC TRANSFOR MATIONSINFe31 6Mn6 5Si ALLOY

１．ＩｎｔｒｏｄｕｃｔｉｏｎＡｃｃｏｒｄｉｎｇｔｏｍａｎｙｐｒｅｖｉｏｕｓｓｔｕｄｉｅｓ,ｔｈｅｓｔａｂｉｌｉｔｙｏｆｆ．ｃ．ｃａｎｄｈ．ｃ．ｐｓｔｒｕｃｔｕｒｅｓｉｎＦｅＭｎｏｒＦｅＭｎｂａｓｅａｌｌｏｙｓｄｅｐｅｎｄｓｓｅｎｓｉｔｉｖｅｌｙｏｎｅｉｔｈｅｒｔｈｅＭｎｃｏｎｔｅｎｔｏｒｔｈｅｍａｇｎｅｔｉｃｐｒｏｐｅｒｔｉｅｓｏｆｔｈｅｆ．ｃ．ｃｐａｒｅｎｔｐｈａｓｅ〔１４〕．ＩｎＦｅＭｎａｌｌｏｙｓｃｏｎｔａｉｎｉｎｇ１７～２８ａｔ．％Ｍｎ,ｔｈｅγ→εｔｒａｎｓｆｏｒｍａｔｉｏｎｓ…     

La0.3Sr0.7FeO3薄膜的输运和光诱导特性研究

采用射频(RF)磁控溅射法制备稀土掺杂铁氧化物La0.3Sr0.7FeO3(LSFO)薄膜。电阻-温度关系表明,薄膜在测量温度范围内呈现半导体导电特性,其主要源于Fe3+和Fe5+离子的电荷有序排列,同时薄膜在250K时发生电荷有序态转变。激光作用诱导薄膜电阻减小,且光致电阻相对变化在190K时取得极大值为56.3%。利用变程跳跃模型对电阻温度曲线进行分析讨论,表明激光作用的内在机制是激光辐照诱导电子退局域化。     

Effects of substituting Ni with M (M=Cu, Al and Mn) on microstructures and electrochemical characteristics of La-Mg-Ni system (PuNi3-type) electrode alloys

In order to improve the electrochemical cycle stability of La-Mg-Ni system (PuNi3-type) hydrogen storage alloy, Ni in the alloys was partially substituted by M (M=Cu, Al, Mn). A new La-Mg-Ni system electrode alloys La0.7Mg0.3Ni2.55-xCo0.45Mx (M=Cu, Al, Mn;x =0,0.1) were prepared by casting and rapid quenching. The effects of element substitution and rapid quenching on the microstructures and electrochemical performances of the alloys were investigated. The results by XRD, SEM and TEM show that the alloys havea multiphase structure, including the (La, Mg)Ni3 phase, the LaNi5 phase and the LaNi2 phase. The rapid quenching and element substitution have an imperceptible influence on the phase compositions of the alloys, but both change the phase abundance of the alloys. The rapid quenching significantly improves the composition homogeneity of the alloys and markedly decreases the grain size of the alloys. The Cu substitution promotes the formation of an amorphous phase in the as-quenched alloy, and a reversal result by the Al substitution. The electrochemical measurement indicates that the element substitution decreases the discharge capacity of the alloys, whereas it obviously improves the cycle stability of the alloys. The positive influence of element substitution on the cycle life of the alloys is in sequence Al＞Cu＞Mn, and negative influence on the discharge capacity is in sequence Al＞Mn＞Cu. The rapid quenching significantly enhances the cycle stability of the alloys, but it leads to a different extent decrease of thedischarge capacity of the alloys.     

颗粒尺寸对多晶La2／3Ca1／3Mn1-xCuxO3低场磁电阻的影响

采用溶胶-凝胶法制备了不同颗粒尺寸的La2/3Ca1/33Mn1-xCuxO3(x=0.04)系列试样。X射线衍射实验说明Cu掺杂和不同温度烧结没有改变晶体的结构。电阻-温度实验曲线表明，随颗粒尺寸的减少，半导体-金属转变温度（Tp）向低温方向移动。磁电阻曲线显示，随颗粒尺寸的减少，与颗粒晶界有关的磁电阻在25K恒温、0.4T低场下由25%增加到了51%。实验结果表明，在La2/3Ca1/3MnO3中少量Cu掺杂和小颗粒尺寸可以实质性地提高与颗粒晶界有关的低场磁电阻效应。     

稀土材料La—Ba—（Mn,Fe）—O的磁电输运特性探讨

研究制备了Ｌａ０．６７Ｂａ０．３３Ｍｎ１－ｘＦｅｘＯ３（ｘ＝０,０．０５,０．１）材料。结果表明：铁替换锰降低了材料的饱和磁化强度及居里温度,主要是因为Ｆｅ离子不参加双交换作用,同时Ｍｎ＾３＋－Ｏ＾３－Ｍｎ＾４＋的作用对随铁离子替代Ｍｎ＾３＋而数量减少,材料的铁磁作用随之减弱。铁替换降低了金属－半导体转换峰温度,相应提高了材料的零场电阻值。值得注意的是铁掺杂提高了大磁阻材料Ｌａ０．６７Ｂａ０．３３Ｍｎ１－ｘＦｅｘＯ３的低温性能,５Ｋ下磁阻比「Ｒ（６Ｔ）－Ｒ（０）」Ｒ（０）从ｘ＝０时的－４０％增加到ｘ＝０．１时的－６０％。本文同时利用迪尼模型对材料大磁阻效应进行了计算分析,发现理论计算曲线可以较好的反映实验上出现的金属－半导体转换峰现象,同时负的大磁阻效应现象也可从理论计算上得到证实。     

A2B7型贮氢合金相结构及电化学性能研究

采用感应熔炼方法制备La0.75Mg0.25Ni3.5-xMnx(x=0,0.05,0.1,0.15,0.2)四元贮氢合金,系统地研究合金B侧Mn对Ni部分替代对合金相结构及电化学性能的影响。XRD分析表明,La0.75Mg0.25Ni3.5-xMnx由La2Ni7相(包括Gd2Co7型高温相和Ce2Ni7型低温相)组成。此外,Mn的加入,使该类合金中出现LaNi5相,但是在含Mn量较高(x=0.15,0.2)的合金中LaNi5相消失。电化学测试表明,随Mn含量的增加,合金电极活化次数变化不大,合金电极的最大放电容量减小,高倍率放电性能、交换电流密度变差,循环稳定性、极限电流密度均得到明显的改善。     

硼添加对La-Mg-Ni-Co系贮氢电极合金的微结构及电化学性能的影响

系统研究了贮氢电极合金La0.7Mg0.3Ni2.65Co0.75Mn0.1Al0.2B,x(x=0,0.02,0.04,0.08)的微结构与电化学性能.XRD结果显示,所有合金均由(La,Mg)Ni3相与LaNi5相组成,B含量的增加导致(La,Mg)Ni,3相的丰度不断增加,相应地LaNi5相的丰度逐渐下降.此外,合金的晶格参数与晶胞体积均随B含量的增加而减小.电化学测试分析表明,B的添加可以显著改善合金电极的高倍率放电性能,当B含量为0.04时达到最佳.微量B的加入对合金的循环稳定性能与活化性能影响很小,但降低合金电极的最大放电容量.此外还采用线性极化与阳极极化对合金电极的动力学性能进行了进一步研究.     

Ni52Mn21+xGa27-x(x=0-5)磁性形状记忆合金的相变

研究了非化学计量成分的多晶Ni52Mn21+xGa27-x(x=0-5)系列合金的热弹性马氏体相变和磁相变.合金的马氏体相变温度Ms随Mn含量的增加而升高,当x＞4时,Ms已经升高到室温以上,而马氏体相变滞后△T随z的增大而减小;合金的磁相变温度TC随z增加而升高,但变化范围不大,在z＞2后,Tc保持在348 K左右.实验获得了一种具有实用前景的合金成分--Ni52Mn25Ga23合金,其马氏体相变温度在室温以上,相变滞后仅为5 K.     

Study on magnetism of Pr0.45（Ca1-xSrx）0.55MnO3 samples

The polycrystalline samples of Pr_0.45(Ca_1−x Sr _x )_0.55MnO₃ (x = 0.0, 0.2, 0.4, 0.6) were prepared by solid-state reaction. Influence of Sr²⁺ substitution for Ca²⁺ at A site on magnetism was studied through the measurements of X-ray diffraction (XRD) spectrum, the magnetization-temperature (M-T) curves and electron spin resonance (ESR) curves. The results show that the magnetism strengthens and charge ordering weakens gradually with the increase of Sr²⁺ substitution amount, respectively. The transition of paramagnetism(PM)-antiferromagnetism(AFM) occurs below the transition temperature of charge ordering (T _CO), and there is little ferromagnetic phase in the antiferromagnetic background at the lower temperature, which results in complex magnetic phases of the samples. Ferromagnetic clusters appear and grow larger with the increase of substitution amount. In addition, the reentrant spin-glass behavior appears at about 41 K. The magnetism phenomenon of the samples is mainly due to the competition between double exchange and Jahn-Teller coupling. The Jahn-Teller coupling becomes weak, and the double exchange wins the advantage in the competition with the increase of substitution amount, which leads to the magnetism variation of the system.     

Effects of ferrites on magnetic transport properties in La2/3Sr1/3MnO3/ferrites composites

Effects of soft-magnetic MnZn ferrite (Mn0.5Zn0.5Fe2O4, MZF) and hard-magnetic Ba ferrite (BaO·6Fe2O3, BaM) on the structure and magnetic transport properties of [La2/3Sr1/3MnO3] (LSMO)/(x) [ferrites] (ferrites=MZF, BaM) composites have been investigated. It was found that the inclusion of MZF phase reduces magnetization and ferromagnetic-paramagnetic transition temperature (Tc) of the composites. With increasing the content of the dopants, the high-temperature magnetoresistance (MR) decreases, whereas low-...     

Structure and electrochemical properties of low-cobalt La1- xLixNi3.2Co0.3Al0.3(0≤x≤0.2) hydrogen storage electrode alloys

The structure and electrochemical properties of a new low cobalt hydrogen storage electrode alloys La1-xLixNi3.2Co0.3Al0.3(0≤ x ≤0.2) were investigated with a different additions of Li in replacement of La. With the increase of Li contents the maximum discharge capacity increases from 240 mAh·g -1 ( x =0) to 328.4 mAh·g -1(x=0.1) and the cycle stability is improved correspondingly. The capacity decay can remaiN28.6% ( x =0.2) after 230 charge/discharge cycles. The high rate discharge(HRD) ability of the alloys( x≤0.1) is improved and the best HRD is 34.1%( x =0.1) under the discharge current density 1200 mA·g -1 . It is found that the prepared alloys are basically composed of LaNi5 as matrix phase and LaNi3 as second phase( x ≤0.1). But the abundance of LaNi3 phase dramatically decreases with increasing x . When x =0.2, a new phase Al(NiCo)3 is formed.     

SPS制备Mn1.1Fe0.9P0.8Ge0.2Bx化合物磁热性能的研究

利用MA+SPS技术制备Mn1.1Fe0.9P0.8Ge0.2Bx(x=0,0.02,0.03,0.04)化合物并对其晶体结构和磁热性能进行研究。XRD分析结果表明:该系列化合物具有六方Fe2P结构。随着B含量的增加晶格常数a和c均发生了明显的变化,导致c/a的值先减小后增大。分别利用DSC和VSM对材料的磁热性能进行了测试,结果表明居里温度TC和熵变均与B的含量存在一个非线性关系,当B的含量为0.02时Mn1.1Fe0.9P0.8Ge0.2B0.02化合物的磁热性能最好,TC从x=0时的253K增加到263K,相应的滞后从23K下降到19K,在0~2T外磁场下的磁熵变从28.7J/kg·K增加到32.6J/kg·K。     

Emissivity of La1-xSrxMnO3/acrylic Resin Thermal Control Coating

Thermal control coatings were fabricated by mixing of La1-xSrxMnO3(LSMO)powder and acrylic resin and brushed on Al alloy substrate.The powders of La0.7Sr0.3MnO3 and La0.8Sr0.2MnO3 were prepared using sol-gel method.XRD results reveal the phase structure of LSMO powders are perovskite.The transition temperature from metal to insulator of La0.7Sr0.3MnO3 and La0.8Sr0.2MnO3 are 300 and 275 K,respectively.The emissivity evolution with temperature of the coatings was measured.For La0.7Sr0.3MnO3/acrylic resin coating,the emissivity increases from 0.56 to 0.88,and for La0.7Sr0.3MnO3/acrylic resin coating from 0.50 to 0.90.     

STRUCTURAL AND MAGNETIC PROPERTIES OF ( PrxSm1 - x ) Mn2Si2

１ＩＮＴＲＯＤＵＣＴＩＯＮＴｅｒｎａｒｙｌａｙｅｒｅｄｉｎｔｅｒｍｅｔａｌｉｃｃｏｍｐｏｕｎｄｓＲＭｎ２Ｘ２（Ｒ＝ｒａｒｅｅａｒｔｈａｎｄＸ＝Ｓｉ,Ｇｅ）ｈａｖｅｂｅｃｏｍｅｏｆｒｅｎｅｗｅｄｉｎｔｅｒｅｓｔｒｅｃｅｎｔｌｙｂｅｃａｕｓｅｏｆｔｈｅｌ...     

La0.7Ce0.3Ni3.75Mn0.35Al0.15Cu0.75-xFex合金的相结构和电化学储氢性能（英文）

采用感应熔炼和热处理的方法制备La0.7Ce0.3Ni3.75Mn0.35Al0.15Cu0.75?xFex(x=0~0.20)合金,并研究合金的相结构和电化学储氢性能。全部合金均为单一的具有CaCu5结构的LaNi5相,LaNi5相的晶格常数a和晶胞体积随着x值的增加而增大。最大放电容量随着x值的增加从319.0mA·h/g(x=0)降低到291.9mA·h/g(x=0.20)。在1200mA/g的电流密度下HRD值从53.1%(x=0)降低到44.2%(x=0.20)。合金电极的循环稳定性随着x值的增加而增强,这主要归因于合金抗粉化能力的增强。     

Magnetic and anomalous transport properties in Fe2MnAl

This study investigated the magnetism and anomalous transport properties of the melt-spun ribbon Fe₂MnAl alloy. It is found that the alloy exhibits ferromagnetic order with the Curie temperature of ∼150 K, followed by another magnetic transition at T_R ∼ 51 K. It is suggested there is antiferromagnetism pinning effect on the ferromagnetic matrix at the temperature below T_R. A steep rise of the resistance below T_R has been observed, which can be understood in terms of antiferromagnetic scattering. An appearance of the resistance maximum near the Curie temperature and the negative temperature dependence of the resistance above Curie temperature are associated with the magnetic phase transition from ferromagnetism to paramagnetism. A negative magnetoresistance at low temperature arising from inhomogeneous magnetic scattering is reported.     

La0．7Mg0．3Ni3．4-xCo0．6Mnx（x=0．0～0．5）贮氢电极合金的结构、储氢特性及电化学性能

La0．7Mg0．3Ni3．4-xCo0．6Mnx(x=0．0～0．5)合金主要由(La，Mg)Ni3相和LaNi5相构成，各相的晶胞参数和晶胞体积均随Mn含量的增加而增大。随Mn含量的增加，合金的放氢平衡压力从0．128MPa(x=0．0)下降到0．067MPa(x=0．5)，导致最大吸氢量从x=0．0时的1．19％(质量分数，下同)逐渐增加到x=0．4时的1．38％。合金的最大放电容量随Mn含量的增加首先从330．4mAh／g（x=0．0)增加到360．6mAh／g(x=0．4)，然后减小到346．9mAh／g(x=0．5)。随Mn替代量的增加，合金电极的高倍率放电能力先改善后降低，合金电极的表面反应阻抗先降低后升高，而氢的扩散系数先增加后减小，说明合金的电化学动力学性能首先提高然后降低。     

(Mn1-xFex)5Sn3合金晶体结构和居里温度

用粉末冶金法(磁场压制烧结)制备(Mn1-xFex)5Sn3(x=0.1～0.5)合金,对其晶体结构、居里温度进行研究。室温XRD分析表明,该系列合金均保持Mn5Sn3的InNi2型相结构,计算发现合金的晶格常数随着x量增大而减小。通过M-T曲线测量结果表明:居里温度TC在室温附近244～391K连续可调,且随着Fe含量的增加而提高,居里温度随成分近似呈线性变化;成分为(Mn0.70Fe0.30)5Sn3合金的居里温度为295K,在外加磁场为0～1.5T下,最大磁熵变约为0.87J·(kg·K)-1,是一种成本低廉的室温磁制冷候选材料。