Yoshida Lab Tatsuo Kano

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Yoshida Lab Tatsuo Kano First-principles calculation of electronic structure of YBa2Cu3O6+y by using the self-interaction correction method Yoshida Lab Tatsuo Kano

Contents Introduction First-principles calculation Kohn-Sham Theory LDA(Local Density Approximation) YBa2Cu3O6+y Methods SIC(Self Interaction Correction) Previous research My work Summary

First-principles calculation Introduction First-principles calculation Predict physical properties of materials ← Input parameters: Atomic Number and Atomic position No external parameters (experimental values) required. Not depend on the model. Advantage ・Low costs ・Extreme conditions ・Ideal environment

Success of First-principles calculation Introduction Success of First-principles calculation Calculated atomic volume (lattice constant) as a function of atomic number. Etotal Emin 笠井秀明,赤井久純,吉田博 編 ; 「計算機マテリアルデザイン」(大阪大学出版会) r (lattice constant) a O

Introduction Kohn-Sham Theory 交換相関エネルギー ψi(r) ? veff(r)

LDA(Local Density Approximation) Introduction LDA(Local Density Approximation) We do not know the vxc and we need approximate expressions of them to perform electronic structure calculations. For a realistic approximation, we refer homogeneous electron gas. Local Density Approximation (LDA) 交換相関エネルギー When the electron density changes in the space, we assume that the change is moderate and the electron density is locally homogeneous.

YBa2Cu3O6+y Superconductivity Electrical resistance → 0 Introduction YBa2Cu3O6+y Superconductivity Electrical resistance → 0 Meissner effect 1911 Hg (4.2K) 1986 La-Ba-Cu-O(30K) 1987 YBa2Cu3O6+y (90K) La-Ba-Cu-O 内部磁場 0 J.G.Bednorz and K.A.Muller ; Z.Physik B64,189 (1986) YBa2Cu3O7-δ http://www.riken.go.jp/r-world/info/release/press/2010/100423/detail.html M.K. Wu et al. Phys. Rev. Letters,  58 908 (1987)

Phase diagram YBa2Cu3O6+y Oxygen Introduction 6.0 6.5 7.0 these samples have a hole doping per planar copper atom of P=0.1 N.Doiron-Leyraud et al. Nature 447, 565-568 (31 May 2007)

Introduction LDA error LDA(Local Density Approximation) error may occur magnetic and strongly-correlated systems. Underestimation of lattice constant. Underestimation of band gap energy. Occupied localize states (d states) at too high energy. Eg(LDA) Eg(expt) M(LDA) M(expt) YBa2Cu3O6 1.7eV 0.1 0.48 P. Wei, Z. Qing ; Phys. Rev. B49, 12159 (1994) Warren E. Pickett ; Rev. Mod. Phys. 61, 433 (1989)

SIC(Self Interaction Correction) Methods SIC(Self Interaction Correction) LDA error can be attributed to the presence of the self-interaction (SI) in the LDA energy function. The SI is present in systems characterized by spatially localized electron charges such as 2p,3d, and 4f electrons. A. Filippetti, N. A. Spaldin, Phys. Rev. B67, 125109 (2003)

A. Filippetti, N. A. Spaldin, Phys. Rev. B67, 125109 (2003) Methods 実験は角度分解光電子分光 A. Filippetti, N. A. Spaldin, Phys. Rev. B67, 125109 (2003)

YBCO crystal structure Previous research YBCO crystal structure Y O Cu Ba YBa2Cu3O6+y(simple tetragonal) YBa2Cu3O7(simple orthorhombic )

YBCO(LDA) Previous research O6は実験ではAFinsulator L. S. Elfimov et al. Phys. Rev. B 77, 060504(R) (2008)

YBCO(SIC) Previous research AF YBa2Cu3O6 PM YBa2Cu3O7 M=0.45μB Gap ~ 1.5eV G. M. Lopez et al. Phys. Rev. B 82, 195122 (2010)

Phase diagram YBa2Cu3O6+y Oxygen Previous research 6.0 6.5 7.0 N.Doiron-Leyraud et al. Nature 447, 565-568 (31 May 2007)

Oxygen doping super-cell method Previous research G. M. Lopez et al. Phys. Rev. B 82, 195122 (2010)

CPA(Coherent Potential Approximation) B AxaBxb A B xa xb + =

My work I calculate electronic structure of YBCO using the self-interaction correction method with KKR-CPA changing oxygen doping. I calculate TN and observe magnetic state.

Summary LDA is a reasonable method in electronic structure calculations, but error may occur magnetic and strongly-correlated systems. SIC is one of the solutions for LDA error. YBa2Cu3O6+y change electronic properties for oxygen doping. I calculate electronic structure of YBCO using SIC changing oxygen doping.