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H.Sakakibara et al., PRB-85, 064501 (2012) H.Sakakibara et al., PRB-89, 224505 (2014) MORISHITA Naoki Kusakabe laboratory M1 Division of Frontier Materials.

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Presentation on theme: "H.Sakakibara et al., PRB-85, 064501 (2012) H.Sakakibara et al., PRB-89, 224505 (2014) MORISHITA Naoki Kusakabe laboratory M1 Division of Frontier Materials."— Presentation transcript:

1 H.Sakakibara et al., PRB-85, 064501 (2012) H.Sakakibara et al., PRB-89, 224505 (2014) MORISHITA Naoki Kusakabe laboratory M1 Division of Frontier Materials Science, Department of Material Engineering Science Graduate School of Engineering Science, Osaka University

2  Introduction ◦ Superconductivity and superconductors  Theoretical models and approaches ◦ Conventional Modeling: The Single-orbital Model ◦ New Modeling : The Two-orbital model ◦ Sakakibara’s Rule  Summary Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 2/15

3 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 3/15 Introduction Phenomena ・ zero resistivity ・ Meissner effect ・ pinning effect ・ Josephson effect Temperature ( K ) Resistivity ( Ω ) Applications ・ power line ・ linear motor train ・ NMR/MRI ・ SQUID

4 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 4/15 Introduction Block layer(s) Buffer layer(s)

5 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 5/15 Introduction liquid nitrogen temperature 77(K)↓ 30(K) (1986) 90(K) (1987) 135(K) (1993) 153(K) (under high-pressure) (2013) 166(K)!? (under high-pressure) (2005) http://sakaki.issp.u-tokyo.ac.jp/user/kittaka/contents/others/tc-history.html

6 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 6/15 Theoretical models and approaches Wannierized wave functionWhole structure on the Cu-O plane Conventional Modeling

7  The Hubbard model(single-orbital) Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 7/15 Theoretical models and approaches 0.15 holes per site = optimal doping ( 最適ドープ ) Conventional Modeling We know much about superconductivity of this model.

8 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 8/15 Theoretical models and approaches H.Sakakibara et al., PRB-85, 064501 (2012) Conventional Modeling

9 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 9/15 Theoretical models and approaches ◆:Theory (single-orbital model) H.Sakakibara et al., PRB- 89, 224505(2014) 25 7575 100 50 ● ● Conventional Modeling

10 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 10/15 Theoretical models and approaches New Modeling H.Sakakibara et al., PRB-85, 064501 (2012)

11  Two-orbital model Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 11/15 Theoretical models and approaches Bad for S.C. / (^o^) \ Good for S.C. \ (^o^) / New Modeling

12 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 12/15 Theoretical models and approaches H.Sakakibara et al.,PRB- 89, 224505(2014) New Modeling

13 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 13/15 Theoretical models and approaches H.Sakakibara et al.,PRB- 89, 224505(2014) (a)Theory(b)Experiment New Modeling

14 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 14/15 Theoretical models and approaches Our aim Large(→bad nesting…)Small(→good nesting!)

15 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ. 15/15 Thank you for your kind attention!

16 Kusakabe lab., Graduate School of Engineering Science, Osaka Univ.


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