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排序方式: 共有29条查询结果,搜索用时 15 毫秒
1.
Two series of Cd1-xInx NNi3(0 ≤x≤ 0.2) and Cd1-yCuyNNi3(0≤y≤0.2) samples were prepared from CdO, In2O3 , CuO, and nickel powders under NH3 atmosphere at 773K. The structural and physical properties were investigated by means of X-ray powder diffraction temperature-dependent resistivity and magnetic measurements. X-ray powder diffraction results showed that the Cd 1 x In x NNi 3 and Cd 1 y Cuy NNi 3 compounds have a typical antiperovskite structure, and the CdNNi3, Cd0.9 In 0.1 NNi3 , and Cd0.9Cu0.1NNi3 compounds show metallic temperature-dependent resistivity and exhibit a Fermi liquid behavior at low temperature. In contrast to the paramagnetism previously reported, the CdNNi 3 sample exhibits very soft and weak ferromagnetism, and no superconductivity was found in the Cd 1 x In x NNi 3 and Cd 1 y Cu y NNi 3 samples down to 2 K. Each sample exhibited very soft and weak ferromagnetism, and the temperature dependence of the magnetization of the Cd 1-xInx NNi 3 and Cd1-y Cu y NNi 3 samples can be well fitted to the combination of a Bloch term and a Curie–Weiss term.  相似文献   
2.
在对系列La 掺杂的Bi2Sr2 - xLaxCuO6 + δ单晶的研究中,我们发现在极度La 掺杂( 空穴极度欠掺杂) 的样品中有高达36K 的超导相出现.X 射线衍射图(XRD) 和电镜照片都表明这种极度空穴欠掺的样品有很好的单相性,从而排除了样品化学不纯的可能.另外,对这种样品进行脱氧处理后,此超导电性相应消失,说明了这种高Tc 的超导电性是由活动性空穴掺杂引起的.虽然对相应样品在正常态的磁测量没有测出反铁磁峰(Neel 峰) ,但对系列样品的拉曼散射研究发现样品随着La 含量的增多,其反铁磁交换作用明显加强.所以,我们认为这种高Tc 超导电性的出现是在Bi2201 体系中存在宏观相分离的明显迹象  相似文献   
3.
Two series of Cdl-xInxNNi3 (0 〈 x 〈 0.2) and Cd1_yCuyNNi3 (0 〈 y 〈 0.2) samples were prepared from CdO, In203, CuO, and nickel powders under NH3 atmosphere at 773 K. The structural and physical properties were investigated by means of X-ray powder diffraction temperature-dependent resistivity and magnetic measurements. X-ray powder diffraction results showed that the Cd1-xInxNNi3 and Cd1_yCuyNNi3 compounds have a typical antiperovskite structure, and the CdNNi3, Cd0.9In0.1NNi3, and Cd0.9Cu0.1NNia compounds show metallic temperature-dependent resistivity and exhibit a Fermi liquid behavior at low temperature. In contrast to the paramagnetism previously reported, the CdNNi3 sample exhibits very soft and weak ferromagnetism, and no superconductivity was found in the Cd1-xInxNNi3 and Cdl-yCuyNNi3 samples down to 2 K. Each sample exhibited very soft and weak ferromagnetism, and the temperature dependence of the magnetization of the Cd1-xInxNNi3 and Cd1_yCuyNNi3 samples can be well fitted to the combination of a Bloch term and a Curie-Weiss term.  相似文献   
4.
为阐明磁性离子在不同替代位置对YBCO体系超导电性的影响机制,利用正电子湮没及相关实验手段结合数值模拟,系统研究了Fe和Ni掺杂的YBa2Cu3O7-δ体系. 结果表明,Fe和Ni离子在替代过程中均以离子团簇的形式进入晶格. 当离子进入CuO2面时,由于团簇改变了周围的电子结构,造成电子的局域化,并直接影响了电子对的配对和输运,因而强烈抑制了体系的超导电性.而当掺杂离子进入Cu-O链区时,它们同样通过团簇的形式改变周围 关键词: YBCO超导体 磁性离子替代 正电子湮没 数值模拟  相似文献   
5.
利用熔融KOH和Co3O4在较低温度(480℃)下反应制备出K0.36CoO2,然后用高锰酸钾溶液和饱和的过硫酸钾溶液进行氧化处理.氧化的同时伴随有水分子嵌入.K0.36CoO2用高锰酸钾和过硫酸钾溶液处理后分别得到K0.12CoO2·0.8H2O和K0.16CO2·0.6H2O.这两种化合物都属于六角晶系,表现出金属行为,脱水后主相变为正交结构并且呈现出半导体特性.K0.16CoO2·0.6H2O在56K附近可能存在自旋玻璃转变行为或其他涨落.随着钾含量的减少和水含量的增多,样品的自旋玻璃行为受到抑制或发生磁性相分离.样品K0.12CoO2·0.8H2O在零场冷却和有场冷却曲线上的分叉现象基本上消失.还讨论了产生KxCoO2与NaxCoO2体系结构和物性差别的原因.  相似文献   
6.
A convenient method for synthesis of tetragonal FeS using iron powder as iron source, is reported. Nanocrystalline tetragonal FeS samples were successfully synthesized by reacting metallic iron powder with sodium sulfide in acetate buffer solution. The obtained sample is single-phase tetragonal FeS with lattice parameters a = 0.3767 nm and c = 0.5037 nm, as revealed by X-ray diffraction. The sample consists of fiat nanosheets with lateral dimensions from 20 nm up to 200 nm and average thickness of about 20 nm. We found that tetragonal FeS is a fairly good conductor from the electrical resistivity measurement on a pellet of the nanosheets. The temperature dependence of conductivity of the pellet was well fitted using an empirical equation wherein the effect of different grain boundaries was taken into consideration. This study provides a convenient, economic way to synthesize tetragonal FeS in a large scale and reports the first electrical conductivity data for tetragonal FeS down to liquid helium temperature.  相似文献   
7.
以K2WO4、WO3和W粉为原料,用混合微波方法制备了钾钨青铜KxWO3样品.随着名义钾含量x的增加,KxWO3样品的晶体结构由六方(0.20≤x≤0.33)转变为四方(0.50≤x≤0.60).四方相样品均显示金属型导电特性.在六方相样品K0.2WO3中观测到了明显的电荷密度波(CDW)转变,转变温度为265K,其余六方相样品则为半导体型导电特性.在x=0.20不变的条件下,以Ca部分替代K制备了(K1-2 yCay)0.2WO3(名义钙含量y=0.1,0.2,0.3)样品,其主相仍为六方相.当0y≤0.2时,六方相的晶胞参数a和c随y的增加而增大.从电阻率-温度曲线上可以看出,名义钙含量的变化会影响样品中的CDW转变.  相似文献   
8.
利用X射线衍射(XRD)和交流磁化率(ACχ)方法系统地研究了Y1x-EuxBa2Cu3O7-δ(x=0.0-1.0)超导体,研究发现Eu 掺杂替代了Y晶位后引起晶格失想与电流密度有密切的联系,对于不同掺杂成分样品,X射线衍射线分析表明(006)及(007)衍射峰型随掺杂量变化,杂浓度在30%和70%附近时,半高宽(FWHM)再现极大值,表明此时样品的晶格失配最大,与此相对应,电流密度Js也在此掺杂浓度范围内达到极大值,我们在晶格失配应力场的钉钆模型下对实现现象进行了讨论,认为Y1-xEuxBa2Cu3O7-δ超导体中由元素替代引起的晶格失配应力场是有效的钉扎中心。  相似文献   
9.
<正>We find that the superconductivity in the thin films of the formerly believed non-superconducting parent compound FeTe is accompanied by an emergence of second order with a correlation length of 742 nm and 258 nm at 10 K and 300 K,respectively.The structural phase transition found in iron pnictide superconductors,in non-superconducting FeTe bulk samples,and in FeSe superconducting thin films is not observed in the superconducting FeTe thin films.The interplay between superconductivity and long range order may suggest the crucial role of competition between electronic localization and itinerancy which leads to strong quantum fluctuations in the FeTe system.  相似文献   
10.
用Cu_2O合成Y-123超导体的研究兰玉成中国科学院物理研究所车广灿,吴非,陈红,贾顺莲,董成,赵忠贤中国科学院物理所超导实验室,北京1000801995年11月27日收到一、引言众所周知,在高Tc氧化物超导体中,[CU-O]p层或[Cu-O]p链?..  相似文献   
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