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Review of typical behaviours observed in strongly correlated systems Charles Simon Laboratoire CRISMAT, CNRS and ENSICAEN, F14050 Caen. Models in magnetism: from basics aspects to practical use Timisoara september 2009 Some examples


  1. Review of typical behaviours observed in strongly correlated systems Charles Simon Laboratoire CRISMAT, CNRS and ENSICAEN, F14050 Caen. “Models in magnetism: from basics aspects to practical use” Timisoara september 2009

  2. Some examples of strongly correlated electrons • Superconductivity • Magnetism • Low dimensionnality • Heavy fermions • Mott insulators models in magnetism timisoara 2

  3. Free electrons 25 20 E F 15 10 5 0 -4 -2 0 2 4 x K Temperature effects (E F =1eV = 30 000K) Band structure (tight binding calculations) models in magnetism timisoara 3

  4. Effect of electron electron repulsion U From T. Giamarchi models in magnetism timisoara 4

  5. Not so strong Effect of correlations Broadening models in magnetism timisoara 5

  6. 6 Photoemission models in magnetism timisoara

  7. Photoemission in insulators Hubbard satellite U models in magnetism timisoara 7

  8. Strongly correlated metal Peak of quasi particules Hubbard peak models in magnetism timisoara 8

  9. Transport properties • Specific heat Cp: • Sommerfeld expansion: models in magnetism timisoara 9

  10. 10 Heavy fermions models in magnetism timisoara

  11. Band mass and effective mass models in magnetism timisoara 11

  12. De Haas Van Alphen effect • In presence of magnetic field, it appears oscillations periodic in 1/H related to the extremum area of the Fermi surface. • In addition, there is a magnetic field dependence of the amplitude related to effective mass. (high mass, high field). models in magnetism timisoara 12

  13. 13 models in magnetism timisoara From JP Brison

  14. Resistivity in T 2 The prefactor A scales with γ 2 condcutivity=ne 2 τ /m Also magnetic susceptibility is Cte From R. Fresard models in magnetism timisoara 14

  15. Thermoelectric power S S= k/e π 2 /2 T/T F (1 + 2/3 z) From Behnia et al. models in magnetism timisoara 15

  16. 16 models in magnetism timisoara

  17. Why oxides ? • Metal U/t small, no correlations, screening of interactions by excitations electron-hole • Oxides Effective t can be small U/t large models in magnetism timisoara 17

  18. Oxides are interesting models in magnetism timisoara 18

  19. Mott insulators V 2 O 3 models in magnetism timisoara 19

  20. Mott insulators V 2 O 3 models in magnetism timisoara 20

  21. 21 models in magnetism timisoara

  22. Organic conductor from Limelette et al. Transfer of the spectral weight models in magnetism timisoara 22

  23. 23 models in magnetism timisoara

  24. 24 Kondo effect models in magnetism timisoara

  25. Kondo effect Magnetic impurities models in magnetism timisoara 25

  26. DMFT • Dynamical mean field theory • To put together quasiparticules and Hubbard states • Limit: no Q dependence, cluster DMFT… models in magnetism timisoara 26

  27. 27 models in magnetism timisoara From A. Georges

  28. Cobaltates Ca 3 Co 4 O 9 From Limelette models in magnetism timisoara 28

  29. 29 Specific heat models in magnetism timisoara

  30. 30 Nickelates RNiO 3 models in magnetism timisoara

  31. Cuprates • They are high Tc superconducting materials Two different scales of energies models in magnetism timisoara 31

  32. Overdoped cuprate: normal Fermi liquid models in magnetism timisoara 32

  33. 33 From B. Vignolle models in magnetism timisoara

  34. YBaCuO underdoped YBa 2 Cu 3 O 6.5 (p = 0.1) A= 5.1 nm -2 = 1.9 % of the carriers Fermi arcs Abnormal photoemission models in magnetism timisoara 34

  35. Fermi surface reconstruction: small pockets models in magnetism timisoara 35

  36. 36 models in magnetism timisoara

  37. 37 models in magnetism timisoara

  38. Other interpretation: stripes models in magnetism timisoara 38

  39. 39 models in magnetism timisoara Cuprates

  40. Manganites Pr 0.7 Ca 0.3 MnO 3 Electronic phase separation ? ? 4 4 30K 30K M ( μ B /f.u.) M ( μ B /f.u.) 3 3 2 2 1 1 0 0 1 1 0 0 10 10 ISOLANT ISOLANT 7 7 R ( Ω ) R ( Ω ) 10 10 METAL METAL 4 4 10 10 1 1 10 10 10 - 10 - 2 2 Jahn Teller effect = orbital ordering 0 0 2 2 4 4 6 6 8 8 10 10 B (T) B (T) Colossal magnetoresistance models in magnetism timisoara 40

  41. From C. Martin From D. Saurel 4 10 30K -1 ) -4 Q Intensity (cm 2 10 2T -2 Q 0 10 4T -3 -2 -1 10 10 10 Q (Å) 0.6 0.6 H S H S H I-M H I-M A nano (a.u.) A nano (a.u.) 0.4 0.4 -1 ) -1 ) S/V ( μ m S/V ( μ m 0.2 0.2 0.0 0.0 2 2 3 3 4 4 5 5 6 6 7 7 Magnetic field (T) Magnetic field (T) From R. Sopracase models in magnetism timisoara 41

  42. Conclusions • Effects of correlations: Fermi surface, effective mass, … – Specific heat, conductivity, magnetic susceptibility, photoemission and dHvA effects • Mott transition, Kondo effects – Phase separation, transfer of spectral weight • Effects of low dimensions models in magnetism timisoara 42

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