Opening… 1 1.

Slides:



Advertisements
Similar presentations
A DFT (LDA+U) Study of the Electronic Properties of Square-Planar Coordinated
Advertisements

Electron-Phonon Interaction in the Polymeric Superconductor, Polysulfur Nitride, (SN) x Paul M. Grant IBM Research Staff Member, Emeritus Session P8: Focus.
A new class of high temperature superconductors: “Iron pnictides” Belén Valenzuela Instituto de Ciencias Materiales de Madrid (ICMM-CSIC) In collaboration.
Iron pnictides: correlated multiorbital systems Belén Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC) ATOMS 2014, Bariloche Maria José.
Soft phonon mode and superconducting properties of 2H-NbS2
The “normal” state of layered dichalcogenides Arghya Taraphder Indian Institute of Technology Kharagpur Department of Physics and Centre for Theoretical.
High Temperature Superconductivity: D. Orgad Racah Institute, Hebrew University, Jerusalem Stripes: What are they and why do they occur Basic facts concerning.
Concepts in High Temperature Superconductivity
 Single crystals of YBCO: P. Lejay (Grenoble), D. Colson, A. Forget (SPEC)  Electron irradiation Laboratoire des Solides Irradiés (Ecole Polytechnique)
Electronic structure of La2-xSrxCuO4 calculated by the
Superconductivity in Zigzag CuO Chains
Spin Waves in Stripe Ordered Systems E. W. Carlson D. X. Yao D. K. Campbell.
Rinat Ofer Supervisor: Amit Keren. Outline Motivation. Magnetic resonance for spin 3/2 nuclei. The YBCO compound. Three experimental methods and their.
Charge Inhomogeneity and Electronic Phase Separation in Layered Cuprate F. C. Chou Center for Condensed Matter Sciences, National Taiwan University National.
Semiconductors n D*n If T>0
Free electrons – or simple metals Isolated atom – or good insulator From Isolation to Interaction Rock Salt Sodium Electron (“Bloch”) waves Localised electrons.
What Pins Stripes in La2-xBaxCuO4? Neutron Scattering Group
A1- What is the pairing mechanism leading to / responsible for high T c superconductivity ? A2- What is the pairing mechanism in the cuprates ? What would.
SO(5) Theory of High Tc Superconductivity Shou-cheng Zhang Stanford University.
Investigating the mechanism of High Temperature Superconductivity by Oxygen Isotope Substitution Eran Amit Amit Keren Technion- Israel Institute of Technology.
Paul M. Grant Visiting Scholar, Stanford ( ) IBM Research Staff Member Emeritus EPRI Science Fellow (Retired) Principal, W2AGZ Technologies The.
Microscopic nematicity in iron superconductors Belén Valenzuela Instituto de Ciencias Materiales de Madrid (ICMM-CSIC) In collaboration with: Laura Fanfarillo.
B. Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC)
Setup. Challenges Confronting High Temperature Superconducting Materials: From Nanoscale Theories to Exascale Energy Applications Aging IBM Pensioner.
SLAC NATIONAL ACCELERATOR LABORATORY The Great Quantum Conundrum SLAC 2575 Sand Hill Road Menlo Park, CA USA SLAC Sand Hill Road Menlo Park, CA Paul.
MgB2 Since 1973 the limiting transition temperature in conventional alloys and metals was 23K, first set by Nb3Ge, and then equaled by an Y-Pd-B-C compound.
Superconducting Gap Symmetry in Iron-based Superconductors: A Thermal Conductivity Perspective Robert W. Hill.
Colossal Magnetoresistance of Me x Mn 1-x S (Me = Fe, Cr) Sulfides G. A. Petrakovskii et al., JETP Lett. 72, 70 (2000) Y. Morimoto et al., Nature 380,

Paired electron pockets in the hole-doped cuprates Talk online: sachdev.physics.harvard.edu Talk online: sachdev.physics.harvard.edu.
Journal of Physics: Conference Series 129 (2008)
Setup. A DFT Study of Tetragonal Rocksalt Proxy Copper Monochalcogenide Structures: -- Implications for Possible High-Tc Superconductivity -- Paul M.
2013 Hangzhou Workshop on Quantum Matter, April 22, 2013
Quantum Confinement in Nanostructures Confined in: 1 Direction: Quantum well (thin film) Two-dimensional electrons 2 Directions: Quantum wire One-dimensional.
Electronic Structure of Cubic Copper Monoxides*
Generalized Dynamical Mean - Field Theory for Strongly Correlated Systems E.Z.Kuchinskii 1, I.A. Nekrasov 1, M.V.Sadovskii 1,2 1 Institute for Electrophysics.
Competing Orders, Quantum Criticality, Pseudogap & Magnetic Field-Induced Quantum Fluctuations in Cuprate Superconductors Nai-Chang Yeh, California Institute.
Galvanomagnetic effects in electron- doped superconducting compounds D. S. Petukhov 1, T. B. Charikova 1, G. I. Harus 1, N. G. Shelushinina 1, V. N. Neverov.
KITPC 23/07/07 Gaps and pseudogaps in n and p-type cuprates from infrared spectroscopy. Ricardo LOBO, Andrés SANTANDER-SYRO, Alexandre ZIMMERS, Nicole.
Development of density functional theory for unconventional superconductors Ryotaro Arita Univ. Tokyo/JST-PRESTO.
Raman Scattering As a Probe of Unconventional Electron Dynamics in the Cuprates Raman Scattering As a Probe of Unconventional Electron Dynamics in the.
Setup. 19 – 27 January APS Cal/Nev Section Annual Meeting 1-2 November 2013 CSU Sonoma Rohnert Park, CA A DFT Study of Tetragonal Rocksalt Copper.
Interplay between magnetism and superconductivity in Fe-pnictides Institute for Physics Problems, Moscow, July 6, 2010 Andrey Chubukov University of Wisconsin.
Zlatko Tesanovic, Johns Hopkins University o Strongly correlated.
Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng Bernstein.
Spatially resolved quasiparticle tunneling spectroscopic studies of cuprate and iron-based high-temperature superconductors Nai-Chang Yeh, California Institute.
6/7/2016 Iron Superconductivity !! o Superconducting Gap in FeAs from PCAR o “Minimal” Model of FeAs planes – Different from CuO 2 !! o Multiband Magnetism.
Setup. A DFT Study of Electron-Phonon Coupling in Proxy CuX (X = S, Se, Te) Structures and Its Relationship to Possible Manifestation of Superconductivity.
Dept. of Physics, Yonsei U
Nature, 18 June Electronic Structure of Rocksalt Copper Monoxide Paul M. Grant Visiting Scholar, Stanford University Principal,
Quest for Higher Tc or RTS
Routes for finding superconductors based on structural trends
Paul Michael Patrick Grant
Possible methods of circumventing the 31% efficiency limit for thermalized carriers in a single–band gap absorption threshold solar quantum.
S25 7 Optimal High-TC Superconductivity in Cs3C60
THE EFFECT OF SPIN COATING RATE ON MICROSTRUCTURES OF CUPROUS OXIDE THIN FILM PREPARED BY SOL-GEL TECHNIQUE DEWI SURIYANI BT CHE HALIN School of Material.
Whither High-Tc 30 Years Following Its Discovery?
Search of a Quantum Critical Point in High Tc Superconductors
Fermi Wavevector 2-D projection ky of 3-D k-space dk
T g* g “Real Metal” “Fermi Liquid” What about RTSC?
S.Li (李晟) and Z.Q.Yang (杨中芹)
R. L. Greene Electron-doped Cuprates University of Maryland
Dirac Line Nodes in Inversion Symmetric Crystals C. L. Kane & A. M
UC Davis conference on electronic structure, June. 2009
Were the Basic Physics Underlying High Temperature Superconductivity
Yoshida Lab Tatsuo Kano
Mössbauer study of BaFe2(As1-xPx)2 iron-based superconductors
Superconducting Fluctuations in One-Dimensional Quasi-periodic Metallic Chains
Thermal diffusivity measurement on Nb by
Fig. 1 Crystal structure and superconductivity in fcc fullerides.
Presentation transcript:

Opening… 1 1

Paul M. Grant IBM Research Staff Member, Emeritus A DFT (LDA+U) Study of the Electronic Properties of Layered, Square-Planar Coordinated Copper Monoxide Structures -- Proxies for High Temperature Superconductivity -- Paul M. Grant IBM Research Staff Member, Emeritus Financial Support From: IBM Retiree Pension Fund Prior to 1990 Aging IBM Pensioner 2 2 2

Prelude “Electronic Properties of Rocksalt Copper Monoxide,” APS MAR09-2008-006217, P. M. Grant, Pittsburgh (2009)

Tools QUANTUM-ESPRESSO Suit of Codes “Dial-in” Parameters Hardware DFT (LDA+U) plus electron-phonon Graphics by Tone Kolalj (XCrysDen) www.quantum-espresso.org “Dial-in” Parameters G2 = 40 Ry ρ = 320 Ry Convergence ≤ 10-6 Ry “Smearing” = Methfessel-Paxton Psuedopotentials: Ultrasoft, XC = Perdew-Zunger Cu: 3d94s2 O: 2s22p4 Hardware 3.33 GHz Intel Core i7 – 12 GB+

Findings Basic Asymmetric af-CuO Cell Spin Up

Are There Phonons w/ High-Tc in YBCO? Fig. 38: Pintschovius and Reichardt, in Furrer, ISBN 0-7923-5226-2

Harashima, et al., Physica C263, 257 (1996) Yes -- They’re There! Harashima, et al., Physica C263, 257 (1996) Pyka, et al., PRL 70, 1457, (1993)

Macfarlane, Rosen, Seki, SSC 63, 831 (1987) Raman Spectroscopy of YBCO

Cubic Rocksalt Copper Monoxide a = b = c = 3.905 Å 10

Rocksalt CuO Combined DOS N(E) (states/eV) EF = 16.74 eV eV

Rocksalt CuO BZ X M Γ X X

Rocksalt CuO Bands Note Degeneracies! eV EF Γ X M X Γ X X 13

Rocksalt CuO Band Widths Note Degeneracies! 14

Rocksalt CuO Fermiology 5 8 12 10 15

Rocksalt CuO Fermiology (Combined) Note (Near) Degeneracies! Jahn-Teller Unstable? Alex M? 16

Non-Magnetic Cubic Rocksalt CuO -- Electron-Phonon Properties -- α2F(ω) λ ~ 0.6 – 0.7 Other sc’s… TC (K) λ μ* K3C60 16.3 0.51 - Rb3C6 0 30.5 0.61 Cs3C6 0 47.4 0.72 σ = 0.04 17 17

Square-Planar Copper Monoxide “Film” a = b = 3.905 Å c = 6 x 3.905 = 23.43 Å 18

“Thin Film” Rocksalt CuO Combined DOS N(E) (states/eV) EF = -2.29 eV eV

“Thin Film” CuO BZ X M Z Γ X

“Thin Film” CuO Bands Note Degeneracies! eV EF Γ X M X Γ Z X 21

“Thin Film” CuO Band Widths Note Band Offsets! 22

“Thin Film” CuO Fermiology (Combined) 2kF “Nesting Fermi Lines” → CDW? → SDW? → HTSC?  ~ ? 23

“Rocks” “Films”

“Rocks” “Films”

“Rocks” “Films”

“Rocks” “Films” “Jahn – Teller” “Nesting”

af-CuO c=6*a U~0.001 eV

af-CuO c=6*a U~0.001 eV

af-CuO c=6*a U~0.001 eV

3D phase diagram of overdoped La2-xCexCuO4 with 0.15 ≤ x ≤ 0.19. Shakes & Spins Copacetic, Competitive or Conundrum? That is the question…anon 3D phase diagram of overdoped La2-xCexCuO4 with 0.15 ≤ x ≤ 0.19. Bottom Line: Can studying CuO proxies with DFT + LDA+U + phonons provide the answer? I say “Yes,” but… How to compute λ(SDW)? Size Matters… …and I need a… BIGGER COMPUTER! Pairing associated with quantum critical energy scales in superconducting electron-doped cuprates K. Jin, N. P. Butch, K. Kirshenbaum, J. Paglione, and R. L. Greene* -submitted to Nature- *will answer all questions…