拓扑半金属研究最新进展

凝聚态物理一个重要的研究内容就是,发现新物态,标识新物态,观测、理解并调控它所具有的物理性质以及不同物态之间的相互转变。日常生活中常见的固态、液态和气态就是三种不同的物态。而无处不在的导电金属和不导电的绝缘体又是另外一种物态分类方式。固体能带理论告诉我们,这是通过对固体中电子的排布方式进行分类的。电子在周期性的固体中呈现能带结构,泡利不相容原理使得每个能带只能填充两个自旋反向的电子。再根据能量最低原理,电子按能量高低次序填充能带,如果恰好填满某个能带,与最低未占据能带之间存在有限大小的能量间隙,那就是绝缘体; 如果有能带未填满,部分占据,那就是金属。     

Superconductivity in Topological Semimetal θ-TaN at High Pressure

Recently,θ-TaN was proposed to be a topological semimetal with a new type of triply degenerate nodal points.Here,we report studies of pressure dependence of transport,Raman spectroscopy and synchrotron x-ray diffraction on θ-TaN up to 61 GPa.We find that θ-TaN becomes superconductive above 24.6 GPa with T_c at 3.1 K.The θ-TaN is of n-type carrier nature with carrier density about 1.1 × 10~(20)/cm~3 at 1.2 GPa and 20 K, while the carrier density increases with the pressure and saturates at about 40 GPa in the measured range.However,there is no crystal structure transition with pressure up to 39 GPa,suggesting the topological nature of the pressure induced superconductivity.     

Quantum Oscillations and Electronic Structure in the Large-Chern-Number Topological Chiral Semimetal PtGa

We report the magnetoresistance(MR),de Haas-van Alphen(dHvA) oscillations and the electronic structures of single-crystal PtGa.The large unsaturated MR is observed with the magnetic field B ‖ [111].Evident dHvA oscillations with the B ‖ [001] configuration are observed,from which twelve fundamental frequencies are extracted and the spin-orbit coupling(SOC) induced band splitting is revealed.The light cyclotron effective masses are extracted from the fitting by the thermal damping term of the Lif...     

Electronic structure,Dirac points and Fermi arc surface states in three-dimensional Dirac semimetal Na_3Bi from angle-resolved photoemission spectroscopy

The three-dimensional(3D) Dirac semimetals have linearly dispersive 3D Dirac nodes where the conduction band and valence band are connected. They have isolated 3D Dirac nodes in the whole Brillouin zone and can be viewed as a 3D counterpart of graphene. Recent theoretical calculations and experimental results indicate that the 3D Dirac semimetal state can be realized in a simple stoichiometric compound A_3Bi(A = Na, K, Rb). Here we report comprehensive high-resolution angle-resolved photoemission(ARPES) measurements on the two cleaved surfaces,(001) and(100), of Na_3Bi. On the(001) surface, by comparison with theoretical calculations, we provide a proper assignment of the observed bands, and in particular, pinpoint the band that is responsible for the formation of the three-dimensional Dirac cones. We observe clear evidence of 3D Dirac cones in the three-dimensional momentum space by directly measuring on the k_x–k_y plane and by varying the photon energy to get access to different out-of-plane k_zs. In addition, we reveal new features around the Brillouin zone corners that may be related with surface reconstruction. On the(100) surface, our ARPES measurements over a large momentum space raise an issue on the selection of the basic Brillouin zone in the(100) plane. We directly observe two isolated 3D Dirac nodes on the(100) surface. We observe the signature of the Fermi-arc surface states connecting the two 3D Dirac nodes that extend to a binding energy of ~150 me V before merging into the bulk band. Our observations constitute strong evidence on the existence of the Dirac semimetal state in Na_3Bi that are consistent with previous theoretical and experimental work. In addition, our results provide new information to clarify on the nature of the band that forms the3 D Dirac cones, on the possible formation of surface reconstruction of the(001) surface, and on the issue of basic Brillouin zone selection for the(100) surface.     

Single crystal growth,structural and transport properties of bad metal RhSb_2

We have successfully grown an arsenopyrite marcasite type RhSb2 single crystal, and systematically investigated its crystal structure, electrical transport, magnetic susceptibility, heat capacity, and thermodynamic properties. We found that the temperature-dependent resistivity exhibits a bad metal behavior with a board peak around 200 K. The magnetic susceptibility of RhSb2 shows diamagnetism from 300 K to 2 K. The low-temperature specific heat shows a metallic behavior with a quite small electronic specific-heat coefficient. No phase transition is observed in both specific heat and magnetic susceptibility data. The Hall resistivity measurements show that the conduction carriers are dominated by electrons with ne = 8.62 × 10¹⁸ cm^-3 at 2 K, and the electron carrier density increases rapidly above 200 K without change sign. Combining with ab-initio band structure calculations, we showed that the unusual peak around 200 K in resistivity is related to the distinct electronic structure of RhSb_2. In addition, a large thermopower S(T) about -140 μV/K is observed around 200 K, which might be useful for future thermoelectric applications.     

磁性外尔半金属材料研究现状与展望

外尔半金属是拓扑半金属家族中的一员。理想的外尔半金属费米面附近有且仅有非简并价带和导带形成的孤立能带交叉点,其低能激发准粒子可以用描述手性外尔费米子的外尔方程来刻画。在三维固体中形成外尔半金属态需要破缺时间反演、中心反演以及它们的组合对称操作。外尔点(即能带交叉点)具有拓扑稳定性和确定的手性或磁荷,且左右手性外尔点需成对出现。非磁性外尔半金属TaAs家族材料的发现,使得研究具有手征性的电子态,及其导致的新物性、新现象成为可能。与非磁性外尔半金属相比,磁性外尔半金属可以仅仅具有一对外尔点,是最简单的外尔半金属,有利于物理机理的分析。磁性外尔半金属可用于实现具有本征磁性的量子反常霍尔效应,提供了通过外磁场来调控外尔点及其相关效应的新手段。文章介绍了磁性外尔半金属的理论模型、拓扑数计算等基本原理,简要回顾了一些典型材料的理论计算和实验研究进展,并介绍了磁性拓扑量子化学理论和磁性拓扑材料的高通量计算,最后讨论了磁性外尔半金属的发展前景和未来的研究方向。     

压力诱导酌拓扑绝缘体化合物Bi2Te3常压相的超导性

通过高压电阻测量,发现了拓扑绝缘体化合物BizTe3压力诱导的超导性,在3-6GPa的压力范围内,超导临界温度L约为3K．高压下原位同步辐射的结果证明这个超导相来源于常压相结构．通过霍尔效应的测量,发现超导的Bi2Te3样品的载流子为P型．对高压同步辐射结果Reitveld精修得到的晶格参数和原子位置,并以此进行第一性...     

从反常霍尔效应到量子反常霍尔效应

美国物理学家霍尔 (Edwin H.Hall) 在1879 年发现,当电流垂直于外磁场通过导体时,在导体的垂直于磁场和电流方向的两个边界之间会出现电势差(图1)。这个现象被称作霍尔效应。在当时要理解这一重要的现象还非常困难,因为电子的概念在18年后才被提出来。     

Band Structure of the Non—Oxide Perovskite MgCNi3

Using the self-consistent full-potential linearized augmented plane wave method,we carry out the electronic structure calculations of MgCNi3 in the local spin density approximation(LSDA) of the density-functional theory.The LSDA solution is metal.The magnetic moment on the Ni ion is only 0.014uB.There is a peak in the density of state just below the Fermi energy(Ef),which can be strongly correlated with various instabilities.After including the strong electron-electron correlation effects on the Ni 3d state by the on-site Coulomb interaction correction,the density of state is greatly redistributed.and the peak just below Ef disappears.The magnetic moment on the Ni ion becomes 0.66uB.Both LSDA and LSDA U have shown that the electroic states near the Fermi surface are dominated by the 3d orbital of Ni.