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Hong Ding Institute of Physics, Chinese Academy of Sciences

ARPES studies of unconventional superconductors. Hong Ding Institute of Physics, Chinese Academy of Sciences. Heavy Fermion Physics Workshop, January 9, 2012. Phase diagrams. pnictide SC. heavy fermion SC. organic SC. cuprate SC. Fermi surface mapping of cuprates. Bi 2 Sr 2 CaCu 2 O 8.

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Hong Ding Institute of Physics, Chinese Academy of Sciences

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  1. ARPES studies of unconventional superconductors Hong Ding Institute of Physics, Chinese Academy of Sciences Heavy Fermion Physics Workshop, January 9, 2012

  2. Phase diagrams pnictide SC heavy fermion SC organic SC cuprate SC

  3. Fermi surface mapping of cuprates Bi2Sr2CaCu2O8 Tight binding fitting Large FS, area = 1-x: Luttinger’s theorem

  4. d-wave superconducting gap in cuprates Half-Integer Flux Quantum Effect

  5. Pseudogap in underdoped cuprates

  6. Phase diagram of Ba122 system Electron doping Hole doping Electron-hole asymmetry? M. Neupane et al., PRB 83, 094522 (2011)

  7. ARPES observation of five bands and five FSs

  8. Fermi surface evolution in “122” Heavily OD Slightly OD OPT UD QAF QAF QAF QAF Tc = 3 K Tc = 22 K Tc = 37 K Tc = 26 K Hole doping Parent UD OPT Heavily OD QAF QAF QAF TN = 135 K Tc = 0 K Tc = 11 K Tc = 25 K Tc = 0 K Electron doping

  9. ARPES observation of superconducting gap 2/Tc ~ 7 H. Ding et al., EPL 83, 47001 (2008)

  10. Nodeless SC gap in Ba0.6K0.4Fe2As2 (Tc = 37K) K. Nakayama et al., EPL 85, 67002 (2009) H. Ding et al., EPL 83, 47001 (2008)

  11. - - - + - J1 – J2 model predicts almost isotropic s± gap Order parameters in momentum Space Real space configuration of pairing symmetry local interactions J1- J2 + + pnictides: large J2 and FS topology favor D = D0coskxcosky, s±-wave cuprates: large J1 and FS topology favor D = D0 (coskx–cosky)/2, d-wave K. Seo, A. B. Bernevig, J. Hu PRL 101, 206404 (2008)

  12. Most weak-coupling theories predict anisotropic s± gap I. Mazin PRB 79, 060502 (2009) D.H. Lee EPL 85, 37005 (2009) S. Graser NJP 11, 025016 (2009) when

  13. overdoped Ba0.3K0.7Fe2As2 (Tc ~ 20K) K. Nakayama et al., PRB 83, 020501(R) (2011)

  14. underdoped Ba0.75K0.25Fe2As2 (Tc = 26K) Y.-M. Xu et al., Nature Communications 2, 392 (2011)

  15. Doping dependence of the SC gaps in Ba1-xKxFe2As2 K. Nakayama et al., PRB 83, 020501(R) (2011)

  16. Electron doped BaFe1.85Co0.15As2 (Tc = 25.5K) K. Terashima et al, PNAS 106, 7330 (2009)

  17. kz dependence of SC gaps single gap function Jab = 30 Jc = 5 D2/D1 ≈ Jc/Jab ≈ 0.17 Y.-M. Xu et al., Nature Physics 7, 198 (2011)

  18. “111” - NaFe0.95Co0.05As(Tc = 18K) Z.-H. Liu et al., arXiv:1008.3265, PRB

  19. “11” - FeTe0.55Se0.45 (Tc = 13K)

  20. J1 = -34 J2 = 22 J3 = 6.8 D2/D3 ≈ J2/J3 ≈ 0.3 H. Miao et al., arXiv:1107.0985

  21. (Tl,K)Fe2-xSe2 (Tc ~ 30K) T. Qian et al., PRL (2011)

  22. Isotropic SC gap on electron FS J1 < 0, FM, d-wave is not favored X.-P. Wang et al., EPL 93, 57001 (2011)

  23. Selection Rules of Pairing Symmetry Self-consistent meanfield equation for t-J model Overlap strength between pairing form factor and Fermi surface OS =

  24. Three classes of high-Tc superconductors J1 J2 J2+J3

  25. Three classes of high-Tc superconductors J1 J2 J2+J3

  26. Summary • The SC gap of all iron-based superconductors measured by ARPES can by described approximately by J1-J2-J3 model • A possible unified paradigm of high-Tc superconductivity: • local AFM magnetic exchange • + collaborative FS topology J.-P. Hu and H. Ding, arXiv:1107.1334

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