E or J KT , et al. PRB 2017; PRB 2017 KT and M.Sato arXiv 2018 Z. - - PowerPoint PPT Presentation

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E or J KT , et al. PRB 2017; PRB 2017 KT and M.Sato arXiv 2018 Z. - - PowerPoint PPT Presentation

01/20 E or J KT , et al. PRB 2017; PRB 2017 KT and M.Sato arXiv 2018 Z. Gong, , KT , PRX 2018 Poster-12 KT et al. in preparation Poster-31 02/20 Lightning ( ) Lichtenberg figure Zener diode Plasma display Figures


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SLIDE 1
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SLIDE 2

E or J

KT, et al. PRB 2017; PRB 2017 KT and M.Sato arXiv 2018

  • Z. Gong, …, KT, … PRX 2018

Poster-12 兎子尾 Poster-31 山本

KT et al. in preparation

01/20

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SLIDE 3

Lightning (雷) Zener diode Plasma display Lichtenberg figure

Figures from Wikipedia

02/20

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SLIDE 4

Gap Gap Zener diode Tunneling between Bloch bands

c.f. Bloch’s theorem, 1928 03/20

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SLIDE 5

Yamakawa et al.,

  • Nat. Mat. 2017
  • Y. Taguchi et al., PRB 2000

Experimental observation

Oka, Arita and Aoki, PRL 2003

Theoretical studies

E

Electric field Current

Mott

E

U

Bias Voltage

04/20

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SLIDE 6

E

E

p e

E

Schwinger機構(電子-陽電子対生成)

  • C. Sow et al., Science 2017

Current T

05/20

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SLIDE 7

・ ・ ・

Kondo insulators

c f

Bose Mott insulators CDW insulators Fermionic Mott ins. Universality in breakdown (Noneq. phase transition)… ? Fermionic Hubbard (1D) Integrable (Bethe ansatz)

: Numerical(DMRG) : Analytical

Oka and Aoki, PRB 2010

c.f. 06/20

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SLIDE 8

・ ・ ・

Kondo insulators

c f

Bose Mott insulators CDW insulators Fermionic Mott ins. Universality in breakdown (Noneq. phase transition)… ? Fermionic Hubbard (1D) Integrable (Bethe ansatz)

: Numerical(DMRG) : Analytical

Oka and Aoki, PRB 2010

c.f. 06/20

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SLIDE 9

KT, M. Nakagawa, N. Kawakami, in prep.

I F

Fth

Insulator Metal Threshold

07/20

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SLIDE 10

G.S. Excited states G.S. 1st ex.

c.f. T. Oka and H. Aoki, PRB 2010

08/20

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SLIDE 11

Outline

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SLIDE 12

Outline

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SLIDE 13

H(t)

“Critical time”

Dykhne-Davis-Pechukas (DDP) 公式

Dykhne, Sov. Phys. JETP 1962 Davis and Pechukas, J. Chem. Phys. 1976

09/20

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SLIDE 14

: Landau-Zener model

“Critical time” LZ formula

Re t Im t

tc

ReE t E

10/20

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SLIDE 15

Outline

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SLIDE 16

Setup:

,

A= ih

F

Fth

Threshold

11/20

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SLIDE 17

A= ih

e+h e-h

Gap closing

Energy gap

h (Asymmetry) hc

=Mott breakdown

c.f. Hubbard case: (proposed by Fukui and Kawakami)

Fukui and Kawakami, PRB 1998

c.f. Random potential → Hatano-Nelson model

Hatano and Nelson, PRL 1996

12/20

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SLIDE 18

A= ih

e+h e-h

Gap closing

Energy gap

h (Asymmetry) hc

=Mott breakdown

c.f. Hubbard case: (proposed by Fukui and Kawakami)

Fukui and Kawakami, PRB 1997

c.f. Random potential → Hatano-Nelson model

Hatano and Nelson, PRL 1996

・非対称ホッピングの冷却原子系での実現提案 ・非エルミート系におけるトポロジカル相

[Ref. Z. Gong, …, KT, … ,M. Ueda, Phys. Rev. X 8 031079 (2018)]

12/20

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SLIDE 19

Outline

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SLIDE 20

h (Asymmetry)

hc

c.f. Giamarchi’s text book

13/20

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SLIDE 21

Sine-Gordon

|g| 14/20

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SLIDE 22

Main result

15/20

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SLIDE 23

ドープされたエルミートな絶縁体へマップされた

16/20

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SLIDE 24

h hc

*Schematic figures

,

17/20

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SLIDE 25

Analytic formula of threshold field

Landau-Zener

t E

β=2 : Band insulator velocity interaction

  • 2. 具体的な模型ではなく有効場の理論にのみ依る

18/20

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SLIDE 26

Fermionic Mott (Hubbard) CDW insulator (XXZ) Band insulator (SSH)

/Δ0

Check:

弱結合領域で幅広く成立している

19/20

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SLIDE 27

KT, M. Nakagawa, N. Kawakami, in prep.

I F

Fth

Insulator Metal Threshold

20/20