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Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets

Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets. Shaffique Adam Cornell University. PiTP/Les Houches Summer School on Quantum Magnetism, June 2006 . For details: S. Adam, M. Kindermann, S. Rahav and P.W. Brouwer, Phys. Rev. B 73 212408 (2006).

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Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets

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  1. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets Shaffique Adam Cornell University PiTP/Les Houches Summer School on Quantum Magnetism, June 2006  For details: S. Adam, M. Kindermann, S. Rahav and P.W. Brouwer, Phys. Rev. B 73 212408 (2006)

  2. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets PiTP/Les Houches Summer School on Quantum Magnetism, June 2006 

  3. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets PiTP/Les Houches Summer School on Quantum Magnetism, June 2006  Quantum Magnetism

  4. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets PiTP/Les Houches Summer School on Quantum Magnetism, June 2006  QuantumMagnetism Electron Phase Coherence

  5. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets PiTP/Les Houches Summer School on Quantum Magnetism, June 2006  QuantumMagnetism Electron Phase Coherence Ferromagnets

  6. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets PiTP/Les Houches Summer School on Quantum Magnetism, June 2006  QuantumMagnetism Electron Phase Coherence Ferromagnets Phase Coherent Transport in Ferromagnets

  7. Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets PiTP/Les Houches Summer School on Quantum Magnetism, June 2006  QuantumMagnetism Electron Phase Coherence Ferromagnets Phase Coherent Transport in Ferromagnets • Motivation (recent experiments) • Introduction to theory of disordered metals • Analog of Universal Conductance Fluctuations in nanomagnets

  8. Motivation: Picture taken from Davidovic group Cu-Co interface are good contacts

  9. Physical System we are Studying [2] • Aharanov-Bohm • contribution • Spin-Orbit Effect Data/Pictures: Y. Wei, X. Liu, L. Zhang and D. Davidovic, PRL (2006)

  10. Physical System we are Studying [3] Aharanov-Bohm contribution Spin-Orbit Effect

  11. V I A Introduction to Phase Coherent Transport Smaller and colder! Image Courtesy (L. Glazman) Sample dependent fluctuations are reproducible (not noise) Ensemble Averages Need a theory for the mean <G> and fluctuations <GG> [Mailly and Sanquer, 1992]

  12. Classical Contribution Quantum Interference Introduction to Phase Coherent Transport [2] Electron diffusing in a dirty metal Impurities Electron Diffuson Cooperon

  13. Introduction to Phase Coherent Transport [3] Weak Localization in Pictures

  14. Introduction to Phase Coherent Transport [3] Weak Localization in Pictures

  15. Introduction to Phase Coherent Transport [3] Weak Localization in Pictures For no magnetic field, the phase depends only on the path. Every possible path has a twin that is exactly the same, but which goes around in the opposite direction. Because these paths have the same flux and picks up the same phase, they can interfere constructively. Therefore the probability to return to the starting point in enhanced (also called enhanced back scattering). In fact the quantum probability to return is exactly twice the classical probability

  16. Classical Contribution Quantum Interference Introduction to Phase Coherent Transport [4] Weak Localization in Equations Cooperon Diffuson

  17. Universal Conductance Fluctuations [Mailly and Sanquer (1992)] [C. Marcus] Theory: Lee and Stone (1985), Altshuler (1985)

  18. Review of Diagrammatic Perturbation Theory (Kubo Formula) Conductance G ~ Diffuson Cooperon Cooperon defined similar to Diffuson upto normalization

  19. Calculating Weak Localization and UCF Weak Localization Universal Conductance Fluctuations

  20. Calculation of UCF Diagrams Sum is over the Diffusion Equation Eigenvalues scaled by Thouless Energy Quasi 1D can be done analytically, and 3D can be done numerically: Var G = 0.272 x 4 for spin

  21. Effect of Spin-Orbit (Half-Metal example) [1] Energy Ferromagnet Fermi Energy Spin Up Spin Down DOS(E) DOS(E) Half Metal

  22. Effect of Spin-Orbit (Half-Metal example) [2] Without S-O With S-O NOTE: For m=m’, Spin-Orbit does not affect the Diffuson (classical motion) but large S-O kills the Copperon (interference)

  23. Calculation of C(m,m’) in Half-Metal Without S-O With S-O m m’ m m = m’ m’ = =

  24. Results for Half-Metal D=1, Analytic Result D=3, Done Numerically We can estimate correlation angle for parameters and find about five UCF oscillations for 90 degree change

  25. Full Ferromagnet Half Metal Ferromagnet

  26. Results for C(m,m’) in Ferromagnet Limiting Cases for m = m’

  27. Conclusions: Showed how spin-orbit scattering causes Mesoscopic Anisotropic Magnetoconductance Fluctuations in half-metals (This is the analog of UCF for ferromagnets) This effect can be probed experimentally

  28. Backup Slides Magnetic Properties of Nanoscale Conductors Shaffique Adam Cornell University

  29. Backup Slide Aharanov-Bohm contribution Spin-Orbit Effect

  30. DOS(E) Energy Fermi Energy Backup Slide Density of States quantifies how closely packed are energy levels. DOS(E) dE = Number of allowed energy levels per volume in energy window E to E +dE DOS can be calculated theoretically or determined by tunneling experiments Fermi Energy is energy of adding one more electron to the system (Large energy because electrons are Fermions, two of which can not be in the same quantum state).

  31. Energy DOS(E) Fermi Energy Spin Down Energy Spin Up Fermi Energy DOS(E) DOS(E) Backup Slide

  32. Backup Slide • Magnetic Field shifts the spin up and spin down bands Energy Ferromagnet Fermi Energy Spin Up Spin Down DOS(E) DOS(E) Spin DOS Half Metal

  33. Backup Slide Weak localization (pictures) For no magnetic field, the phase depends only on the path. Every possible path has a twin that is exactly the same, but which goes around in the opposite direction. Because these paths have the same flux and picks up the same phase, they can interfere constructively. Therefore the probability to return to the starting point in enhanced (also called enhanced back scattering). In fact the quantum probability to return is exactly twice the classical probability

  34. Classical Contribution Quantum Interference Backup Slide Weak localization (equations) Diffuson Cooperon

  35. Backup Slide Weak Localization and UCF in Pictures <G> <G G>

  36. Backup Slide

  37. Backup Slide

  38. Backup Slide

  39. Backup Slide Introduction to Quantum Mechanics Energy is Quantized Wave Nature of Electrons (Schrödinger Equation) Scanning Probe Microscope Image of Electron Gas (Courtesy A. Bleszynski) Wavefunctions of electrons in the Hydrogen Atom (Wikipedia)

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