EuSr2Ru1-xTaxCu2O8体系的超导电性和磁性质

通过对EuSr2Ru1-xTaxCu2O8(x=0, 0.1, 0.2, 0.5和1.0)体系的结构、电阻和磁化强度的观测,结果发现:EuSr2RuCu2O8(x=0)样品在130.2K以下呈现铁磁有序,在10K时发生了超导转变,并呈现典型的欠掺杂高温超导体特征,随着Ta对Ru替代浓度x值的增加,铁磁相变温度和超导临界温度均下降.同时,对该体系中的元素替代效应,及其磁有序和超导电性的共存进行了详细讨论.     

High-Pressure Single-Crystal Neutron Scattering Study of Magnetic and Fe Vacancy Orders in （T1,Rb）：Fe4Se5 Superconductor

The recently discovered metal-intercalated iron selenide superconductors A2Fe4Se5 （A=K, Cs, T1- K, Rb, T1-Rb） （245） compounds, with Tc ～30K, have attracted much interest A high transition- temperature （TN ≈ 470-560K） and large magnetic moment （3.3μB/Fe） block antiferromagnetic （AFM） order exists in the superconducting samples. Mag- netic order-parameter experiences an anomaly when Tc is approached. The superconductors crystal- lize with a highly ordered √5 × √5 superstructure, in which the Fel site of the I4/m structure is only a few percents occupied and the Fe2 site is fully occupied. The non-superconducting samples at low-T also crystallize in the I4/m structure, while both Fe sites are fractionally occupied, since the numbers of the Fe vacancies in the samples and the vacant sites in the √5 × √5 pattern are mismatched. The partially ordered √5× √5 vacancy order becomes one of three competing phases for temperature below room temperature up to ～ 500K, namely, these sam- ples are phase-separated and in the miscibility gap 1lacier the n,mhi~nt condition.     

Exploration of iron-chalcogenide superconductors

Iron-chalcogenide compounds with FeSe（Te, S） layers did not attract much attention until the discovery of high-Tc superconductivity （SC） in the iron-pnictide compounds at the begining of 2008. Compared with FeAs-based superconductors, iron-chalcogenide superconductors have aroused enormous enthusiasm to study the relationship between SC and magnetisms with several distinct features, such as different antiferromagnetic ground states with relatively large moments in the parents, indicating possibly different superconducting mechanisms, the existence of the excess Fe atoms or Fe vacancies in the crystal lattice. Another reason is that the large single crystals are easily grown for the iron-chalcogenide compounds. This review will focus on our exploration for the iron-chalcogenide superconductors and discussion on several issues, including the crystal structure, magnetic properties, superconductivity, and phase separation. Some of them reach a consensus but some important questions still remain to be answered.     

Co(S1-xSex)2系统中的铁磁量子相变

针对Co(S1-xSex)2系统在x=0.11附近发生的铁磁金属到顺磁金属相变,制备了一系列不同Se替代浓度的多晶样品.通过对其结构和电阻率-温度ρ(T)关系的系统观测,结果发现,样品铁磁相变温度TC随着Se替代浓度x值的增加,以(1-x)1/2关系单调下降,其二级铁磁相变转变为一级相变;在临界浓度x=0.11附近,其ρ(T)关系由Fermi液体行为转变为非Fermi液体行为.作者认为,Co(S1-xSex)2系统在x=0.11附近发生的是一种量子相变,在该量子相变点附近零温度下的自旋量子涨落导致其ρ(T)关系的反常行为.     

Magnetoresistance and Kondo Effect in Nodal-Line Semimetal VAs_2

We performed calculations of the electronic band structure and the Fermi surface,measured the longitudinal resistivity ρxx(T,H),Hall resistivity ρxy(T,H),and magnetic susceptibility as a function of temperature at various magnetic fields for VAs₂ with a monoclinic crystal structure.The band structure calculations show that VAs₂ is a nodal-line semimetal when spin-orbit coupling is ignored.The emergence of a minimum at around11 K in ρxx(T) measured at H=0 demonstrates that some additional magnetic impurities(V⁴⁺,S=1/2)exist in VAs₂ single crystals,inducing Kondo scattering,evidenced by both the fitting of ρxx(T) data and the susceptibility measurements.It is found that a large positive magnetoresistance(MR) reaching 649% at 10 K and 9 T,its nearly quadratic field dependence,and a field-induced up-turn behavior of ρxx(T) also emerge in VAs₂,although MR is not so large due to the existence of additional scattering compared with other topological nontrivial/trivial semimetals.The observed properties are attributed to a perfect charge-carrier compensation,which is evidenced by both the calculations relying on the Fermi surface and the Hall resistivity measurements.These results indicate that the compounds containing V(3d³4s²) element can be as a platform for studying the influence of magnetic impurities to the topological properties.     

Bi2Sr2Co2O8体系中Pb替代及I插层对其结构和物性的影响

自今年3月在NaxCo2O4 Yh2o中发现超导电性以来,具有层状结构的Co系氧化物又受到人们广泛的关注.本文在成功合成具有misfit层状结构Bi2Sr2Co2Oy单相样品的基础上,通过Pb对Bi的部分替代、以及I的插层,成功地使其c轴由1.49nm增至1.87nm,并对其输运性质和磁性质进行了系统研究.结果发现:Pb的部分替代并没有使该体系的电阻-温度关系行为发生显著变化,但在低温下使样品呈现自旋玻璃态行为;I的插入不仅使其c轴长度增加,而且样品变为半导体,并不呈现超导电性,在低温下同样呈现自旋玻璃态行为.同时对Pb替代及I插层效应进行了讨论.     

Sr2Fe1-xCoxMoO6体系中Co的元素替代效应

在成功制备具有双钙钛矿结构Sr2Fe1-xCoxMoO6系列样品的基础上,对其结构、输运性质和磁性质进行了系统研究.结果发现,随着Co替代浓度x值的增加,样品的电阻率-温度关系由半金属行为转变为半导体行为,其室温电阻率从3.9×10-5Ω·cm增大到6.0×10-1Ω·cm;样品由亚铁磁体转变成反铁磁体,其磁相变温度TN值也随之下降;Co对Fe的部分替代使其磁电阻效应受到抑制.基于对其电子结构的分析,其磁电阻效应的起源以及Co的元素替代效应也在文中进行了讨论.     

Na0.75Co1-xRuxO2体系中的金属-绝缘体相变

在采用固相反应法成功制备单相Na0.75Co1-xRuxO2(0≤x≤0.5)样品的基础上,对其结构、输运性质和磁性质进行了系统研究.结果表明, x≤0.5的样品仍保持单相,样品的晶格参数随着Ru替代浓度x值的增加逐渐增大,说明在该体系中,Ru能均匀地替代Co.对于x=0的样品,在整个测量温区内,其电阻率-温度关系呈现典型的金属行为; x=0.01样品在T=37K附近发生了金属-绝缘体相变;而x≥0.02的所有样品,整个测量温区内均为半导体.与x=0样品相比较,x=0.1样品在30K时的电阻率增大了5个数量级.我们认为该体系在x=0.01附近发生的金属-绝缘体(MI)相变,起源于CoO2层的无序导致的电子的Anderson局域化.对于所有样品,在2K以上均没有观测到长程磁有序,其磁化率在100 K以上均满足居里-外斯定律,同时对该体系的磁化率结果进行了详细讨论.     

EuSr2Ru1—xTaxCu2O8超导电性和磁性系的体质

通过对EuSr2Ru1-xTaxCu2O8(x=0，0．1，0．2，0．5和1．0)体系的结构、电阻和磁化强度的观测，结果发现：EuSr2RuCuO8(x=0)样品在130．2K以下呈现铁磁有序，在10K时发生了超导转变，并呈现典型的欠掺杂高温超导体特征，随着Ta对Ru替代浓度x值的增加，铁磁相变温度和超导临界温度均下降。同时，对该体系中的元素替代效应，及其磁有序和超导电性的共存进行了详细讨论。     

Na0．75Co1-xRuxO2体系中的金属-绝缘体相变

在采用固相反应法成功制备单相Na0．75Co1-xRuxO2（0≤x≤0．5）样品的基础上，对其结构、输运性质和磁性质进行了系统研究．结果表明，x≤0．5的样品仍保持单相。样品的晶格参数随着Ru替代浓度x值的增加逐渐增大，说明在该体系中，Ru能均匀地替代Co．对于x=0的样品，在整个测量温区内，其电阻率-温度关系呈现典型的金属行为；x=0．01样品在T=37K附近发生了金属-绝缘体相变；而x≥0．02的所有样品，整个测量温区内均为半导体．与x=0样品相比较．x=0．1样品在30K时的电阻率增大了5个数量级．我们认为该体系在x=0．01附近发生的金属-绝缘体（MI）相变，起源于CoO2层的无序导致的电子的Anderson局域化．对于所有样品，在2K以上均没有观测到长程磁有序。其磁化率在100K以上均满足居里-外斯定律，同时对该体系的磁化率结果进行了详细讨论．