363 research outputs found

    High-field Studies on Layered Magnetic and Polar Dirac Metals

    Full text link
    Recently, the interplay between the Dirac/Weyl fermion and various bulk properties, such as magnetism, has attracted considerable attention, since unconventional transport and optical phenomena were discovered. However, the design principles for such materials have not been established well. Here, we propose that the layered material AAMnX2X_2 (AA: alkaline and rare-earth ions, XX: Sb, Bi) is a promising platform for systematically exploring strongly correlated Dirac metals, which consists of the alternative stack of the X−X^- square net layer hosting a 2D Dirac fermion and the A2+A^{2+}-Mn2+^{2+}-X3−X^{3-} magnetic block layer. In this article, we shall review recent high-field studies on this series of materials to demonstrate that various types of Dirac fermions are realized by designing the block layer. First, we give an overview of the Dirac fermion coupled with the magnetic order in EuMnBi2_2 (AA=Eu). This material exhibits large magnetoresistance by the field-induced change in the magnetic order of Eu layers, which is associated with the strong exchange interaction between the Dirac fermion and the local Eu moment. Second, we review the Dirac fermion coupled with the lattice polarization in BaMnX2X_2 (AA=Ba). There, spin-valley coupling manifests itself owing to the Zeeman-type spin-orbit interaction, which is experimentally evidenced by the bulk quantum Hall effect observed at high fields.Comment: 28 pages, 10 figures, published in JPSJ (Special Topics

    Rich structural phase diagram and thermoelectric properties of layered tellurides Mo1-xNbxTe2

    Full text link
    MoTe2 is a rare transition-metal ditelluride having two kinds of layered polytypes, hexagonal structure with trigonal prismatic Mo coordination and monoclinic structure with octahedral Mo coordination. The monoclinic distortion in the latter is caused by anisotropic metal-metal bonding. In this work, we have examined the Nb doping effect on both polytypes of MoTe2 and clarified a structural phase diagram for Mo1-xNbxTe2 containing four kinds of polytypes. A rhombohedral polytype crystallizing in polar space group has been newly identified as a high-temperature metastable phase at slightly Nb-rich composition. Considering the results of thermoelectric measurements and the first principles calculations, the Nb ion seemingly acts as a hole dopant in the rigid band scheme. On the other hand, the significant interlayer contraction upon the Nb doping, associated with the Te p-p hybridization, is confirmed especially for the monoclinic phase, which implies a shift of the p-band energy level. The origin of the metal-metal bonding in the monoclinic structure is discussed in terms of the d electron counting and the Te p-p hybridization.Comment: 16 pages, 6 figures, 1 table, to be published in APL Material

    Modified memoryless spectral-scaling Broyden family on Riemannian manifolds

    Full text link
    This paper presents modified memoryless quasi-Newton methods based on the spectral-scaling Broyden family on Riemannian manifolds. The method involves adding one parameter to the search direction of the memoryless self-scaling Broyden family on the manifold. Moreover, it uses a general map instead of vector transport. This idea has already been proposed within a general framework of Riemannian conjugate gradient methods where one can use vector transport, scaled vector transport, or an inverse retraction. We show that the search direction satisfies the sufficient descent condition under some assumptions on the parameters. In addition, we show global convergence of the proposed method under the Wolfe conditions. We numerically compare it with existing methods, including Riemannian conjugate gradient methods and the memoryless spectral-scaling Broyden family. The numerical results indicate that the proposed method with the BFGS formula is suitable for solving an off-diagonal cost function minimization problem on an oblique manifold.Comment: 20 pages, 8 figure

    Effect of Applied Orthorhombic Lattice Distortion on the Antiferromagnetic Phase of CeAuSb2_2

    Full text link
    We study the response of the antiferromagnetism of CeAuSb2_2 to orthorhombic lattice distortion applied through in-plane uniaxial pressure. The response to pressure applied along a ⟨110⟩\langle 110 \rangle lattice direction shows a first-order transition at zero pressure, which shows that the magnetic order lifts the (110)/(11ˉ0)(110)/(1\bar{1}0) symmetry of the unstressed lattice. Sufficient ⟨100⟩\langle 100 \rangle pressure appears to rotate the principal axes of the order from ⟨110⟩\langle 110 \rangle to ⟨100⟩\langle 100 \rangle. At low ⟨100⟩\langle 100 \rangle pressure, the transition at TNT_N is weakly first-order, however it becomes continuous above a threshold ⟨100⟩\langle 100 \rangle pressure. We discuss the possibility that this behavior is driven by order parameter fluctuations, with the restoration of a continuous transition a result of reducing the point-group symmetry of the lattice.Comment: 6 pages, 7 figure

    Effect of uniaxial stress on the magnetic phases of CeAuSb2_2

    Full text link
    We present results of measurements of resistivity of \CAS{} under the combination of cc-axis magnetic field and in-plane uniaxial stress. In unstressed \CAS{} there are two magnetic phases. The low-field A phase is a single-component spin-density wave (SDW), with q=(η,±η,1/2)\mathbf{q} = (\eta, \pm \eta, 1/2), and the high-field B phase consists of microscopically coexisting (η,η,1/2)(\eta, \eta, 1/2) and (η,−η,1/2)(\eta, -\eta, 1/2) spin-density waves. Pressure along a ⟨100⟩\langle 100 \rangle lattice direction is a transverse field to both of these phases, and so initially has little effect, however eventually induces new low- and high-field phases in which the principal axes of the SDW components appear to have rotated to the ⟨100⟩\langle 100 \rangle directions. Under this strong ⟨100⟩\langle 100 \rangle compression, the field evolution of the resistivity is much smoother than at zero strain: In zero strain, there is a strong first-order transition, while under strong ⟨100⟩\langle 100 \rangle it becomes much broader. We hypothesize that this is a consequence of the uniaxial stress lifting the degeneracy between the (100) and (010) directions.Comment: 8 pages, 7 figure
    • …
    corecore