yosuke harashima , keith slevin department of physics, osaka university, japan

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Numerical analysis for the metal-insulator transition in doped semiconductors using density functional theory in the local density approximation Yosuke Harashima, Keith Slevin Department of Physics, Osaka University, Japan

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Numerical analysis for the m etal-insulator transition in doped semiconductors using density functional theory in the local density approximation. Yosuke Harashima , Keith Slevin Department of Physics, Osaka University, Japan. Metal-insulator transition in doped semiconductors. - PowerPoint PPT Presentation

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Page 1: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Numerical analysis for the metal-insulator transitionin doped semiconductors

using density functional theory in the local density approximation

Yosuke Harashima, Keith SlevinDepartment of Physics, Osaka University, Japan

Page 2: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Metal-insulator transition in doped semiconductors

Disorder

Electron-electron interaction

Metal-insulator transition

ex. Critical exponent

Page 3: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Impurity band for low concentration

Page 4: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

For high concentration

Page 5: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Model

• Donor impurities distributed

randomly in space

• Long range Coulomb interaction for electron-electron pairs

Page 6: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Schrödinger equation for impurity band

= 0.32

= 12.0

Page 7: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Kohn-Sham equations

Auxiliary system:

Page 8: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Exchange-correlation energy in an effective medium

Page 9: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Local density approximation

Page 10: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

In this study M=2 and h=18[Bohr]

Complete spin polarized case (for simplicity)

Real space finite difference approximation

Calculation details

Page 11: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Multi-fractal analysis for Kohn-Sham orbital

A. Rodriguez et al (2011)

Page 12: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

• Extended states:

• Localized states:

Asymptotic behavior

Page 13: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Metal-Insulator Transition around nD ≈ 1.5 [10-7 Bohr-3]

Page 14: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Density of states

• Periodic system • Disordered system

Page 15: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

nD ≈ 0.6 [10-7 Bohr-3]

Page 16: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

nD ≈ 1.4 [10-7 Bohr-3]

Page 17: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

nD ≈ 1.9 [10-7 Bohr-3]

Page 18: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan
Page 19: Yosuke  Harashima , Keith  Slevin Department of Physics, Osaka University, Japan

Summary

The model taking into account, • Random positions of impurities.• Electron-electron interaction using DFT in LDA.

The existence of the Metal-Insulator transition around nD ≈ 1.5 [10-7 Bohr-3] is shown in this model.

We are calculating the critical exponents. As extension, • Spin of electrons using local spin density approximation.• Compensation of impurities.