A Pressure-Induced Emergence of a Weyl Semimetal Phase in Pb1-xSnxTe J

Slides:



Advertisements
Similar presentations
Quantum “disordering” magnetic order in insulators, metals, and superconductors HARVARD Talk online: sachdev.physics.harvard.edu Perimeter Institute, Waterloo,
Advertisements

Ch 9.4: Competing Species In this section we explore the application of phase plane analysis to some problems in population dynamics. These problems involve.
Quantum anomalous Hall effect (QAHE) and the quantum spin Hall effect (QSHE) Shoucheng Zhang, Stanford University Les Houches, June 2006.
© red ©
The Nuts and Bolts of First-Principles Simulation
Topological Insulators and Beyond
1 Material Electromagnetic Property Material partition under electric field Material partition under magnetic field Lorentzian model Artificial material.
The Color Wheel Claire Heider The Primary Colors.
Thermal Boundary Resistance of the Superfluid 3 He A-B Phase Interface D.I. Bradley S.N. Fisher A.M. Guénault R.P. Haley H. Martin G.R. Pickett J.E. Roberts.
Thermodynamics and Kinetics of Phase Transformations in Complex Non-Equilibrium Systems Origin of 3D Chessboard Structures: Theory and Modeling Armen G.
Berry Phase Effects on Electronic Properties
Chapter 2. Coulomb’s law.
Correlated States in Optical Lattices Fei Zhou (PITP,UBC) Feb. 1, 2004 At Asian Center, UBC.
Jeroen van den Brink Bond- versus site-centred ordering and possible ferroelectricity in manganites Leiden 12/08/2005.
If you say 8 color the ones in your picture purple. If you say 9 color the ones in your picture blue.
An Alternative Semiconductor Definition!
Electrons on the brink: Fractal patterns may be key to semiconductor magnetism Ali Yazdani, Princeton University, DMR Princeton-led team of scientists.
Ferroelectricity induced by collinear magnetic order in Ising spin chain Yoshida lab Ryota Omichi.
Stress induced roughening of superclimbing dislocations Anatoly Kuklov, (CSI, CUNY), (DMR-) PHY Boris V. Svistunov, (UMass, Amherst), (DMR-) PHY
Structural Determination of Solid SiH 4 at High Pressure Russell J. Hemley (Carnegie Institution of Washington) DMR The hydrogen-rich solids are.
National Science Foundation Switching in the Presence of Defects Volkmar Dierolf, Lehigh University, DMR Outcome: Researchers at Lehigh University.
CRITICAL DIMENSIONS OF STRONGLY INTERACTING ANISOTROPIC SYSTEMS Babich Artem Institute of Electrophysics and Radiation Technologies NAS of Ukraine.
Theoretical Solid State Physics Marvin L. Cohen and Steven G. Louie, University of California at Berkeley, DMR Carbon nanotubes possess novel properties.
Kinetics of Structural Transformations in Metal and Ceramic Systems Microstructure in Decomposition of Metastable Ceramic Materials Armen G Khachaturyan,
Unconventional superconductivity, where Cooper pairing is driven by something other than electron-phonon coupling, often appears in proximity to magnetic.
Quantum spin Hall effect Shoucheng Zhang (Stanford University) Collaborators: Andrei Bernevig, Congjun Wu (Stanford) Xiaoliang Qi (Tsinghua), Yongshi Wu.
Liquids and Solids. Intermolecular Forces  Intermolecular Forces are the attraction between molecules  They vary in strength, but are generally weaker.
Courtesy of Pr. D. Leinweber, CSSM, University of Adelaide
Boyce/DiPrima 9th ed, Ch 9.4: Competing Species Elementary Differential Equations and Boundary Value Problems, 9th edition, by William E. Boyce and.
Phase Changes Sublimation Deposition.
Some Coordination Compounds of Cobalt Studied by Werner
Light propagation in topological two-level structures
Topological Phase transitions and Topological phases of matter
SEMICONDUCTORS Semiconductors Semiconductor devices
Yosuke Harashima, Keith Slevin
3.1.4 Direct and Indirect Semiconductors
Insulators, Semiconductors, Metals
Band structure: Semiconductor
Magnetism.
PHYSICS 2415 Suggested strategies: Read text before lecture
Average Number of Photons
PHASE DIAGRAMS.
Computational Re-design of Synthetic Genetic Oscillators for Independent Amplitude and Frequency Modulation  Marios Tomazou, Mauricio Barahona, Karen.
Dirac Line Nodes in Inversion Symmetric Crystals C. L. Kane & A. M
Routing Valley Excitons with a Metasurface
Pressure-induced spin-state and insulator-metal transition in Sr2CoO3F by first principles Xue-dong Ou and Hua Wu We have studied the electronic structure.
Correlations of Electrons in Magnetic Fields
Discovery of a Weyl fermion semimetal and topological Fermi arcs
Landau Quantization and Quasiparticle Interference in the
ConcepTest Clicker Questions College Physics, 7th Edition
Chiral anomaly observed as an axial current in two topological quantum materials DMR M. Hirschberger, J. Xiong, S. Kushwaha, A. Bernevig,
Observation of Fermi arc surface states in a topological metal
The chiral anomaly in a Dirac semimetal
He Meng, Johan Bosman, Thijn van der Heijden, John van Noort 
Hysteresis Curves from 11 dimensions
Evidence for the chiral anomaly in the Dirac semimetal Na3Bi
SOC Fermi Gas in 1D Optical Lattice —Exotic pairing states and Topological properties 中科院物理研究所 胡海平 Collaborators : Chen Cheng, Yucheng Wang, Hong-Gang.
Blowing magnetic skyrmion bubbles
Energy Band 7 In free electron model, electrons occupy positive energy levels from E=0 to higher values of energy. They are valence electron so called.
Methods of Charging S Explain attraction of neutral objects using the particle model of electricity. S Explain electrostatic phenomena.
Video .
Fig. 3 Near-field maps of a multiply cracked α-(BEDT-TTF)2I3 crystal.
Fig. 1 Topology and electronic structure of TaAs.
A strongly robust type II Weyl fermion semimetal state in Ta3S2
by Yoshifumi Tokiwa, Boy Piening, Hirale S. Jeevan, Sergey L
Discovery of Lorentz-violating type II Weyl fermions in LaAlGe
by Shuichi Murakami, Motoaki Hirayama, Ryo Okugawa, and Takashi Miyake
T. M. Truskett, D.J. Milliron: University of Texas at Austin
Fig. 4 Optical properties of the modes guided in twisted coreless PCF.
Bulk-boundary correspondence and topological nontrivial nature of TaP
Presentation transcript:

A Pressure-Induced Emergence of a Weyl Semimetal Phase in Pb1-xSnxTe J A Pressure-Induced Emergence of a Weyl Semimetal Phase in Pb1-xSnxTe J. Kim & N. Kioussis (California State University Northridge), DMR-1205734(PREM) T. Liang & Nai Phuan Ong (Princeton University) Outcome: In collaboration with experimental studies at Princeton University we have carried out ab initio calculations to examine the effect of pressure on the topological phase diagram of Pb1-xSnxTe. The calculations reveal that the ferroelectric polarization, which breaks crystal inversion symmetry, induces a Weyl semimetallic state separating the normal insulator and topological crystalline insulator phases. The metallic phase features pairs of Weyl nodes of opposite chiralities which persist over a finite pressure range. Hence the metallic phase is protected since the Weyl nodes cannot be removed except by mutual annihilation which occurs at higher pressure. Impact: The picture of how a gap closes in a semiconductor has been recently radically transformed by topological concepts. Instead of the gap closing and immediately reopening, we predict that in the absence of inversion symmetry, a topological metallic phase protected by Weyl nodes persists over a finite range of pressure. Explanation: The ferroelectric polarization gives rise to a topological phase transition from a normal insulator to a Weyl semimetal to a topological crystalline insulator under external pressure. The twelve Weyl nodes trace out elliptical orbits with increasing pressure and eventually annihilate pairwise at the higher critical pressure. We predict that the number of Weyl points can be tuned by an external magnetic field. a b c d (a) Ferroelectric polarization versus lattice constant phase diagram. The pink (blue) wedge is where the 12 Weyl nodes near the L1, L2, and L3 (L0) points are stable. (b) k-space trajectories of Weyl nodes under pressure where positive (negative) chiralities are colored red (blue). (c) Magnetic field versus lattice constant phase diagram with applied field B || [111]. Orange (yellow) shaded areas denote four (two) Weyl nodes near the L points. (d) Effect of magnetic field on the Weyl node separation. Publication: T. Liang, S. Kushwaha, J. Kim, Q. Gibson, J. Lin, N. Kioussis, R. J. Cava, and N. Phuan Ong, Sci. Adv. 2017; 3: e1602510.