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Berry Phase Effects on Bloch Electrons in Electromagnetic Fields

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Presentation on theme: "Berry Phase Effects on Bloch Electrons in Electromagnetic Fields"— Presentation transcript:

1 Berry Phase Effects on Bloch Electrons in Electromagnetic Fields
Qian Niu 牛谦 University of Texas at Austin 北京大学 Collaborators: Y. Gao, Shengyuan Yang, C.P. Chuu, D. Xiao, W. Yao, D. Culcer, J.R.Shi, Y.G. Yao, G. Sundaram, M.C. Chang, T. Jungwirth, J. Sinova, A.H.MacDonald H. Weitering, J. Beach, M. Tsoi, J. Erskine Supported by : DOE, NSF, Welch Foundation

2 Outline Berry phase and its applications
Berry curvature in momentum space Anomalous velocity, Anomalous Hall effect Density of States, Orbital Magnetization Effective Quantum Mechanics Second order extension Positional shift Magnetoelectric Polarization Nonlinear anomalous Hall effect

3 Berry Phase In the adiabatic limit: Geometric phase:

4 Well defined for a closed path
Stokes theorem Berry Curvature

5 Analogy to Gauge Field Berry curvature Magnetic field
Berry connection Vector potential Geometric phase Aharonov-Bohm phase Chern number Dirac monopole

6 Analogy to Riemann Geometry
Berry curvature Gaussian curvature Berry connection Levi-Civita connection Geometric phase Holonomy angle Chern number Genus

7 Applications Berry phase Berry curvature Chern number interference,
energy levels, polarization in crystals Berry curvature spin dynamics, electron dynamics in Bloch bands Chern number quantum Hall effect, quantum charge pump ``Berry Phase Effects on Electronic Properties”, by D. Xiao, M.C. Chang, Q. Niu, Review of Modern Physics

8 Outline Berry phase and its applications
Berry curvature in momentum space Anomalous velocity, Anomalous Hall effect Density of States, Orbital Magnetization Effective Quantum Mechanics Second order extension Positional shift Magnetoelectric Polarization Nonlinear anomalous Hall effect

9

10 Symmetry properties time reversal: space inversion: both:
violation: ferromagnets, asymmetric crystals

11 Berry Curvature in Fe crystal

12 Anomalous Hall effect velocity distribution g( ) = f( ) + df( )
current Intrinsic

13 Temperature dependence of AHE
J. P. Jan, Helv. Phys. Acta 25, 677 (1952)

14 Experiment Mn5Ge3 : Zeng, Yao, Niu & Weitering, PRL 2006

15 Intrinsic AHE in other ferromagnets
Semiconductors, MnxGa1-xAs Jungwirth, Niu, MacDonald , PRL (2002) , J Shi’s group (2008) Oxides, SrRuO3 Fang et al, Science , (2003). Transition metals, Fe Yao et al, PRL (2004),Wang et al, PRB (2006), X.F. Jin’s group (2008) Spinel, CuCr2Se4-xBrx Lee et al, Science, (2004) First-Principle Calculations-Review Gradhand et al (2012)

16

17 Some Magneto Effects Density of states and specific heat:
Magnetoconductivity:

18 Orbital magnetization
Free energy Xiao, Shi & Niu, PRL 2005 Xiao, et al, PRL 2006 Also see: Thonhauser et al, PRL (2005). Ceresoli et al PRB (2006).

19 Anomalous Thermoelectric Transport
Berry phase correction Thermoelectric transport

20 Thermal Hall Conductivity
Phonon Magnon Electron Wiedemann-Franz Law

21 Effective Quantum Mechanics
Wavepacket energy Energy in canonical variables Quantum theory Spin-orbit Spin & orbital moment Yafet term

22 Outline Berry phase and its applications
Berry curvature in momentum space Anomalous velocity, Anomalous Hall effect Density of States, Orbital magnetization Effective Quantum Mechanics Second order extension Positional Shift Magnetoelectric Polarization Nonlinear anomalous Hall effect

23 Why second order? In many systems, first order response vanishes
May be interested in magnetic susceptibility, electric polarizebility, magneto-electric coupling Magnetoresistivity Nonlinear anomalous Hall effects

24 Positional Shift Use perturbed band:
Solve from the first order energy correction: Modification of the Berry connection – the positional shift

25 Equations of Motion Effective Lagrangian: Equations of motion

26 Magnetoelectric Polarization
Polarization in solids: Correction under electromagnetic fields: Magnetoelectric Polarization:

27 Magnetoelectric Polarization
Restrictions: No symmetries of time reversal, spatial inversion, and rotation about B.

28 Nonlinear anomalous Hall current
Intrinsic current: Results – only anomalous Hall current:

29 Electric-field-induced Hall Effect
Electric field induced Hall conductivity (2-band model):

30 Magnetic-field induced anomalous Hall
Model Hamiltonian: Magnetic field induced Hall conductivity: Compare to ordinary Hall effect

31 Conclusion Berry phase is a unifying concept
Berry curvature in momentum space Anomalous velocities, Anomalous Hall effect Density of states, Orbital magnetization Effective quantum Mechanics Second order extension Positional shift Magnetoelectric polarization Nonlinear anomalous Hall effect


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