Nb对C-15相V2Zr和V2(HfZr)系列声子性能的影响

本文用中子飞行时间方法对C-15相的超导物质V₂Zr,V₂Zr_0.95Nb_0.05及V₂Hf_0.5Zr_0.5,V₂Hf_0.5Zr_0.3Nb_0.2的热中子非弹性散射谱作了测量,发现Nb的添加对V₂Zr和V₂Hf_{0.5 关键词：}     

Ta对C—15相V_2Hf和V_2(Zr_(0.5)Hf_(0.5))系列声子性能的影响

本文用中子飞行时间方法对C-15相的超导材料V_2Hf,V_2Ta和V_2Hf_(0.8)Ta_(0.2)以及V_2Zr_(0.5)。Hf_(0.5)和V_2Zr_(0.5)Hf_(0.33)Ta_(0.17)的热中子非弹性散射谱作了测量,并计算出相对的广义声子态密度。结果与早先发表的Nb对C-15相V_2Zr和V_2(Hf_(0.5)Zr_(0.5))系列声子性能的影响一致:声子频率随超导转变温度T_c增加而软化,随T_c减小而硬化。这表明,对于此类材料弹性软化在一定程度上对提高T_c起了作用。结果还进一步表明V_2Zr或V_2Hf与V_2(Zr_(0.5)Hf_(0.5))之间有着质的差别,V_2Hf加Ta后,T_c增加,声子频率软化,而V_2(Zr_(0.5)Hf_(0.5))加Ta后,T_c减小,声子频率则略有硬化。这与V_2Zr和V_2(Hf_(0.5)Zr_(0.5))加Nb的结果是一致的。此结果可以用角动量分波表象的能带论方法分析电-声耦合相互作用得出的杂化理论来定性解释。     

Nb对C-15相V_2Zr和V_2(HfZr)系列声子性能的影响

本文用中子飞行时间方法对C-15相的超导物质V_2Zr,V_2Zr_(0.95)Nb_(0.05)及V_2Hf_(0.5)Zr_(0.5),V_2Hf_(0.5)Zr_(0.3)Nb_(0.2)的热中子非弹性散射谱作了测量,发现Nb的添加对V_2Zr和V_2Hf_(0.5)Zr_(0.5)系列的作用不同,V_2Zr添加第三组元Nb后,超导临界温度Tc增加,声子频率“软化”,而V_2Hf_(0.5)Zr_(0.5)系列添加第四组元Nb后,Tc略有下降,声子频率则“硬化”。V_2Zr_(0.95)Nb_(0.05)声子频率比V_2Zr“软化”的结果与以前磁化率下降几何平均声子频率上升的结果不一致。对于V_2Hf_(0.5)Zr_(0.5)加Nb后声子频率“硬化”的现象用角动量分波表象的能带论方法分析电-声作用得出的杂化理论作了解释     

Nb对C-15结构V2(HfZr)系列的超导转变温度的影响

本文中研究了C-15结构V₂Hf_1-xNb_x,V₂Zr_1-xNb_x和V₂Hf_0.5Zr_0.5-xNb_x系列的超导转变温度T_c与Nb合量x的关系,发现V₂Zr,V₂Hf加Nb后与V₂Hf_0.5Zr_0.5加Nb后性能显著不同。测定了V₂Zr,V₂Hf和V₂Hf_0.5Zr_0.5的X射线光电子能谱。结果表明,当Hf原子和Zr原子共存于AB₂化合物的A位上时,发生了一种增强原子间相互作用的新的电荷转移。这个事实支持由角动量分波表象能带论方法分析电声耦合超导原理的结果对四元V₂(HfZrNb)系列的超导行为提出的一种可能解释:4d-5d原子配位可能有助于提高4d导带的杂化程度,从而有利于提高超导T_c。 关键词：     

C-15结构(Hf,Zr,Ta)V2和(Hf,Zr,Nb)V2合金超导转变的压力效应研究

本文研究了C-15结构化合物(Zr_0.5Hf_0.5-xTa_x)V₂(x≤0.2)和(Hf_0.5Zr_0.5-xNb_x)V₂(x≤0.2)的超导转变温度T_c及其压力效应?T_c/?P。报道了实验方法与结果。与(Hf_1-xTa_x)V₂和(Zr_1-xTa_x)V₂的情况不同,在(Zr_0.5Hf_0.5-xTa_x)V₂中Ta的引入使常压下的T_c下降,然而(?)T_c/(?)P却大为提高。因此高压下Zr_0.5Hf_0.45Ta_0.05V₂的T_c反而比Hf_0.5Zr_0.5V₂更高。导出了一个基于角动量分波表象能带论方法的描述压力效应的新关系式。它指出导带电子波函数中的高角动量成分变化对T_c的压力效应影响比较重要。这个公式有助于理解上述复杂的实验现象,并能合理地解释某些元素(如Cs,Ba,La等)的T_c随压力剧增的事实。 关键词：     

(Hf0.5Zr0.5V2)Hx的声子谱与超导性的关系

本文报道了用Be过滤探测器谱仪对C-15相的(Hf_0.5Zr_0.5V₂₎H_x等五种样品的声子谱的测量。观察到了它们的声子谱随含氢量而变化以及声学支有规则的软化现象。表明(Hf_0.5Zr_0.5V₂₎H_x的T_c随x的变化,主要是声学支的贡献,声学文软化有利于T_c的提高,而光学支“软化”可能会抑制超导性。 关键词：     

C15相(Hf_0.5—xTa_xZr_0.5)V_2H_y系超导电性研究

对C15相(Hf_0.5-xTa_xZr_0.5)V_2H,系的超导电性研究表明,该系的T_c～y关系及H影响T_c的机制与Pd-H系不同。热中子非弹性散实验的结果表明,声频支对T_c的变化是重要的.根据Jacob和Miedema的理论,对在小浓度和大浓度时,氢在不同间隙位置的分布作了理论分析,似乎当氢原子主要占据2Zr—2V间隙位置时,T_c升高.对此,本文提出一种可能的解释.     

La0.3Sr0.7TiO3模板层对Pb(Zr0.5Ti0.5)O3薄膜的铁电性能增强效应的研究

通过sol-gel法在Si (111) 基片上分别制备了LaNiO₃(LNO)底电极和LaNiO₃/La_0.3Sr_0.7TiO₃ (LNO/LSTO)底电极.然后采用sol-gel 方法，在两种衬底上分别制备了Pb (Zr_0.5Ti_0.5)O₃ (PZT)铁电薄膜.XRD分析表明，两种PZT薄膜均具有钙钛矿结构，且在LNO底电极上的PZT薄膜呈(100) 择优取向，而在LNO/LSTO底电极上的PZT薄膜呈随机取向.铁电性能测试表明，相对LNO衬底上制备的PZT薄膜，在LNO/LSTO底电极上制备的PZT薄膜的剩余极化强度得到了有效的增强，同时矫顽场也增大.介电常数和漏电流的测试表明，LNO/LSTO底电极上制备的PZT薄膜具有大的介电常数和漏电流. 关键词： PZT薄膜 铁电性 漏电流 0.3Sr_0.7TiO₃')" href="#">La_0.3Sr_0.7TiO₃     

V2Ga5的晶体结构

本文利用单晶与粉末衍射方法测定了V₂Ga₅的晶体结构。V₂Ga₅属四方晶系,其单相区约为VGa₂—V₂Ga₅。在18℃的点阵常数是a=8.9540?,c=2.6892?,每个晶胞含有二个化合式量,空间羣为D_4h⁵—P4/mbm。V原子与Ga原子分别占据在4(h)与8(i),2(d)的等效位置上。参数为:x相似文献   

拓扑绝缘体(Bi0.5Sb0.5)2Te3薄膜中的线性磁阻

本文报道了拓扑绝缘体(Bi_0.5Sb_0.5)₂Te₃薄膜中线性磁阻问题的系统性研究工作. 此体系中, 线性磁阻在很宽的温度和磁场范围内出现: 磁场高达18 T时磁阻仍没有饱和趋势, 并且当温度不高于50 K时, 线性磁阻的大小对温度的变化不敏感. 栅压调控化学势可明显改变线性磁阻的大小. 当化学势接近狄拉克点时, 线性磁阻最为显著. 这些结果说明电荷分布的不均匀性是引起该材料线性磁阻的根源.     

INVESTIGATION OF THE EFFECT OF SLOW NEUTRON IRRADIATION ON HALOGEN-DOPED HIGH-Tc SUPERCONDUCTORS AND ITS MECHANISM

Irradiation effect of low-fluence (-10⁸ n/cm² ) slow neutrons on halogen-doped superconductors is presented in this paper. And the mechanism of the effect is also described from the viewpoint of nuclear physics for both fast and slow neutrons on high-temperature superconductors (HTSC). It is shown ex-perimentally and theoretically that slow neutrons of low fluence has a similar irradiation effect to that of fast neutron beams with an energy E_n>0.1 MeV and fluence 10¹⁶-10¹⁸ n/cm²-However,quite differ-ent mechanisms are involved in them: Fast neutrons transfer their energies through elastic scattering in HTSC, whereas slow neutrons give off their energies during the slow neutron capture (n,γ) reaction.     

(GaAs)1(AlAs)1(001)超晶格与闪锌矿结构Ga0.5Al0.5As合金虚晶能带的对应性

基于线性丸盒轨道原子球近似(LMTO-ASA)数值计算,比较(GaAs)₁(AlAs)₁(001)超晶格与闪锌矿结构Ga_0.5Al_0.5As合金虚晶能带本征态,发现它们可以用Ⅲ价和Ⅴ价原子平面的分波态进行统一描述,用这种方法详细分析超晶格与闪锌矿结构合金在布里渊区Γ,M(X)和R(L)诸点主要能带本征态之间的对应关系,讨论了超晶格布里渊区能带折叠对本征态的影响。 关键词：     

Lattice instabilities and superconductivity of (Hf,Zr) V2 compounds

The temperature dependences of the sound velocity of the pseudobinary (Hf, Zr)V₂ compounds show the evidence of lattice instability. The inverse relation between the superconducting transition temperature and the deduced transformation temperature is shown.     

RBa2Cu3Ox(R为稀土元素)超导体中F代O的研究

以CuF₂为配方试剂之一,合成系列掺F稀土超导体RBa₂Cu₃O_xF_y。对比观测发现,稀土氧化物超导体以F代O后,烧结温度明显降低,超导转变宽度变窄,零电阻温度稍有提高,晶胞参数发生变化,F进入123相晶格,文中还讨论掺F效应。 关键词：     

MgB2和Mg0.93Li0.07B2的电阻率与霍尔效应研究

测量了MgB₂和Mg_0.93Li_0.07B₂的电阻率ρ(T)与霍尔系数R_H(T)的温度依赖关系.电阻率的测量结果表明,MgB₂和Mg_0.93Li_0.07B₂的正常态电阻率与温度有平方的依赖关系.MgB₂和Mg_0.93Li_0.07B_{2关键词： 电阻率 霍尔效应}     

Synthesis and properties of a new copper(II)-hafnium phosphate Cu0.5Hf2(PO4)3

Phosphates of general formula M_0.5Hf₂(PO₄)₃ with M=Cd²⁺, Ca²⁺, Sr²⁺ and Cu²⁺ were prepared by coprecipitation and characterized by several physical techniques. The compounds containing Cd²⁺, Ca²⁺, Sr²⁺ belong to the Nasicon-type structure, whereas Cu_0.5Hf₂(PO₄)₃ exhibited substantially different DRX patterns. Combined temperature programmed reduction (TPR) and temperature-programmed oxidation (TPO) showed that the copper in Cu_0.5Hf₂(PO₄)₃ was distributed between two energetically different sites in proportions respectively equal to 40 and 60%. Electron Paramagnetic Resonance (EPR) investigations confirmed the TPR/TPO results and revealed that the two sites hosting the Cu²⁺ ions are of orthorhombic symmetry. Moreover, the Cu²⁺ ions might be reduced by hydrogen to Cu⁺. These results were also supported by the UV–visible studies that showed the disappearance, under reducing conditions, of the band corresponding to crystal field transitions of Cu²⁺ ions and the emergence of a new peak attributed to the transitions between (3d)¹⁰ and (3d)⁹(4s)¹ Cu⁺ levels. At the same time, IR spectroscopy confirmed that protons entered the open lattice framework of the material and gave rise to a new protonated phase containing monovalent copper Cu_0.5^IH_0.5Hf₂(PO₄)₃. This redox process was proven to be reversible without any subsequent change in the network of the phosphate.