Magnetic and Electrical Transport Properties of Sr1-xLaxRuO3 (0≤x≤0.10)

We investigate the lightly doped polycrystalline Sr1-χLaχRuO3 （χ = 0, 0.02, 0.08 and 0.10）. With La doping, the ferromagnetism in the system has been suppressed. The transition temperature is T＇c at which the long-range ferromagnetism establishes and the magnetization under 3 T at 5 K decreases with increasing χ. In contrast to Sr1-χCaχRuO3, the samples remain with the PM-FM transition at 162K, which might be attributed to the valency change of Ru.     

(110)取向La0.67Sr0.33MnO3-δ外延膜的结构和磁电阻效应研究

采用直流磁控溅射法在(110)LaAlO3单晶基片上制备了La0.67Sr0.33MnO3-δ外延膜,系统地研究了样品的结构以及基片温度、外磁场对磁电阻效应的影响.将LSMO/(110)系列样品与LSMO/(001)系列样品的电阻率对比之后,发现基片的不同取向对该系列样品的电输运性质有很大的影响.原因是在不同取向时,氧原子进入薄膜的几率不同,导致Mn+3/Mn+4的比率不同,使得晶格常数、Mn+3和Mn+4与O-2之间的相互作用和原子磁矩的取向发生了变化,从而引起了金属到半导体的转变温度Tp移向高温区域和电阻率明显下降.     

双钙态矿Sr_2Fe_(1-x)Mn_xMoO_6体系的磁性和磁输运性质的研究(英文)

我们用X射线光电子能谱、以及相关的电性和磁性测量研究了Sr2Fe1-xMnxMoO6(0相似文献   

Transient Photoconductivity in LaRhO_3 Thin Film

High-quality epitaxial LaRhO_3(LRO) thin films on SrTiO_3(110) single-crystalline substrates are fabricated by pulsed laser deposition and their photoconductivity properties are studied. The transient photoconductivity(TPC) effect is found in this semiconductor LRO film at room temperature. The magnitude of TPC increases almost linearly with the laser power intensities and the photon energies in visible light range. Moreover, the difference in the TPC results under two airflow conditions confirms that both intrinsic photoinduced carrier accumulation and extrinsic photoinduced heating effects contribute to the magnitude of TPC effect.     

SmFeAsO0.78F0.22中Mn掺杂对超导电性的抑制效应

本文报道了Mn替代Fe对最佳掺杂的Sm-1111体系超导电性的影响.通过电输运及磁性质的测量发现Mn对Fe的替代迅速抑制了超导电性.随着Mn含量的增加,体系的电阻率ρ和磁化率M逐渐增大.对于低掺杂x＜0.25%和未掺杂样品,M接近零,对于≤1%,M从室温到超导转变几乎不变,实验指出Fe2+失去其磁性.我们提出这是由于F...     

Electric and magnetic behaviour in double doped La2/3＋4x/3Sr1/3-4x/3Mn1-xMgxO3

The double-doped La2/3＋4x/3Sr1/3-4x/3Mn1-xMgxO3 samples with fixed Mn^3＋/Mn^4＋ ratio equal to 2/1 are investigated by means of magnetism and transport measurements. Phase separation is observed at temperature higher than T^onset c for x = 0.10 and 0.15. For x = 0.10, rather strong phase separation induces drastic magnetic random potential and results in the localization of carriers. Thus, the varlable-range hopping process dominates. For other samples, there is no or only weak phase separation above T^onset c. Thus, thermal activation mechanism is responsible for the high temperature transport behaviour. For x = 0.20 and 0.25, unexpected AFM behaviour is observed at low temperature. All these results are well understood by considering the special role of the ＂double-doping＂.     

Cr掺杂对BaxSr1-xRuO3体系磁性和输运性质的影响

本文采用固相反应法制备了BaxSr1-xRuO3和BaxSr1-xRu0.9Cr0.1O3两组样品,对比研究了它们磁性和电输运性质.当掺杂量少于0.2时,体系处于有少许畸变的钙钛矿的3C结构,Cr的掺入很大幅度提高了体系的铁磁转变温度Tc,电输运性质上也由坏金属行为转变为Mott绝缘体的行为,并且在铁磁相变附近出现电阻拐点.当掺杂量大于等于0.2时,体系发生结构相变,由畸变钙钛矿3C结构变为6 M的单斜结构.这时,Cr的掺入对体系的影响并不明显.这些结果表明引起SrRuO3铁磁转变温度升高的Ru+5-O-Cr+3相互作用对晶格结构有强烈的依赖关系.     

从FeSe0.5Te0.5的V～I曲线论磁通动力学的诸模型（英文）

高温超导体的发现动摇了支配磁通动力学二十几年的Kim-Anderson模型.于是人们提出了新的涡旋玻璃态模型,集体钉扎模型和U～j对数关系模型来描述高温超导体的磁通动力学.其中,涡旋玻璃态模型已被人们广泛接受.Fe基超导体发现后,人们它行为十分类似于高温超导体.我们实验上仔细研究了FeSe0.5Te0.5单晶的V～I关系曲线,发现上述诸模型均不能很好的解释我们的实验结果,而张的反跳模型恰能很好的拟合实验结果.本文讨论了诸模型对高温超导体磁通动力学描述的适用性并给出合理的解释.     

LPL3层膜的结构、磁性和磁电阻效应的研究

采用直流溅射法在 ( 1 0 0 )LaAlO3 单晶基片上制备了La_0.67Sr_0.33MnO_3+δ/Pr_0.7Ca_0.3MnO_3+δ/La_0.67Sr_0.33MnO_3+δ(简称为LPL) 3层膜 .用X射线粉末衍射法(XRD)研究了系列样品的摇摆曲线和衍射全图 ,结果表明所有的样品均为高度取向的外延膜 .SQUID磁强计的测量结果证实了 3层膜中磁耦合的存在 .用常规的四端引线法测量了LSMO、PCMO和LPL 3层膜的电阻 ,分析了logρ 1 /T曲线 .由此可以得出如下结论 :具有铁磁性的PCMO中间层在 3层膜中可能起到了内磁场的作用 ,使得LSMO膜的顺磁性被削弱 ,这个作用与外加磁场的作用一样 ,降低了 ρ_max,增大了由金属到半导体的转变温度T_p;PCMO中间层还诱发了LSMO的能隙中的态密度的变化 .以上两个原因使得在零场中样品的电阻率和T_p 随着中间层PCMO的厚度变化而明显变化 .