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Antoine Georges Olivier Parcollet Nick Read Subir Sachdev Jinwu Ye

Mean field theories of quantum spin glasses. Antoine Georges Olivier Parcollet Nick Read Subir Sachdev Jinwu Ye. Talk online: Sachdev. Classical Sherrington-Kirkpatrick model. J ij : a Gaussian random variable with zero mean. Two routes to quantization. A. Quantum rotor model.

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Antoine Georges Olivier Parcollet Nick Read Subir Sachdev Jinwu Ye

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  1. Mean field theories of quantum spin glasses Antoine Georges Olivier Parcollet Nick Read Subir Sachdev Jinwu Ye Talk online: Sachdev

  2. Classical Sherrington-Kirkpatrick model Jij : a Gaussian random variable with zero mean

  3. Two routes to quantization A. Quantum rotor model n=1: Ising model is a transverse field g g Spectrum at Jij=0 n=3: randomly coupled spin dimers g Spectrum at Jij=0

  4. Two routes to quantization B. Heisenberg spins Spectrum at Jij=0 (2S+1)-fold degeneracy Generalize model to SU(N) spins and explore phase diagram in N, S plane

  5. Outline • Insulating quantum rotors. • Insulating Heisenberg spins • DMFT of a random t-J model • Metallic spin glasses: DMFT of a random Kondo lattice

  6. A. Insulating quantum rotors

  7. A. Quantum rotor model Jij : a Gaussian random variable with zero mean

  8. Local dynamic spin susceptibility T=0 phases Spin glass Paramagnet Specific heat C ~ T (?) g D.A. Huse and J. Miller, Phys. Rev. Lett.70, 3147 (1993). J. Ye, S. Sachdev, and N. Read, Phys. Rev. Lett.70, 4011 (1993). N. Read, S. Sachdev, and J. Ye, Phys. Rev. B 52, 384 (1995). A. Georges, O. Parcollet, and S. Sachdev, Phys. Rev. B 63, 134406 (2001).

  9. T > 0 phase diagram gc g J. Ye, S. Sachdev, and N. Read, Phys. Rev. Lett.70, 4011 (1993). N. Read, S. Sachdev, and J. Ye, Phys. Rev. B 52, 384 (1995).

  10. B. Insulating Heisenberg spins

  11. B. Heisenberg spin glass Jij : a Gaussian random variable with zero mean S. Sachdev and J. Ye, Phys. Rev. Lett. 70, 3339 (1993).

  12. T=0 phase diagram S Spin glass order Specific heat C ~ T (C ~ T2 ?) N S. Sachdev and J. Ye, Phys. Rev. Lett. 70, 3339 (1993). A. Georges, O. Parcollet, and S. Sachdev, Phys. Rev. Lett. 85, 840 (2000). A. Camjayi and M. J. Rozenberg, Phys. Rev. Lett. 90, 217202 (2003).

  13. Quantum critical phase is described by fractionalized S=1/2 neutral spinon excitations Spinon spectral density w S. Sachdev and J. Ye, Phys. Rev. Lett. 70, 3339 (1993).

  14. T > 0 phase diagram S. Sachdev and J. Ye, Phys. Rev. Lett. 70, 3339 (1993). A. Georges, O. Parcollet, and S. Sachdev, Phys. Rev. Lett. 85, 840 (2000). A. Camjayi and M. J. Rozenberg, Phys. Rev. Lett. 90, 217202 (2003).

  15. C. Doping the quantum critical spin liquid

  16. C. DMFT of a random t-J model Jij : a Gaussian random variable with zero mean O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  17. = carrier density O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  18. Physical consequences of quantum criticality 1. Electron spectral function (photoemission) Momentum resolved spectral density O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  19. Physical consequences of quantum criticality 2. d.c Resistivity O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  20. Physical consequences of quantum criticality 3. NMR 1/T1 relaxation rate O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  21. Physical consequences of quantum criticality 4. Optical conductivity O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  22. Phenomenological phase diagram for cuprates O. Parcollet and A. Georges, Phys. Rev. B 59, 5341 (1999).

  23. D. Metallic spin glasses

  24. C. DMFT of a random Kondo lattice model Jij : a Gaussian random variable with zero mean S. Sachdev, N. Read, and R. Oppermann, Phys. Rev. B 52, 10286 (1995). A. M. Sengupta and A. Georges, Phys. Rev. B 52, 10295 (1995).  

  25. JK S. Sachdev, N. Read, and R. Oppermann, Phys. Rev. B 52, 10286 (1995). A. M. Sengupta and A. Georges, Phys. Rev. B 52, 10295 (1995).  

  26. Outlook • Spin glass order is an attractive candidate for a quantum critical point in the cuprates, on both theoretical and experimental grounds. (Impurities break the translational symmetry associated with charge-ordered states, and the Imry-Ma argument then prohibits a quantum critical point associated with charge order in the presence of randomness in two dimensions) • A simple mean-field theory of a doped Heisenberg spin glass naturally reproduces all the “marginal” phenomenology. • Needed: better theory of fluctuations in low dimensions

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