Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B....

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Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland, 17 th , March, 2010
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Transcript of Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B....

Page 1: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Fermi-Edge Singularityin Tunnel Junctions

Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii

University of Warwick, U.K.

APS March Meeting, Portland, 17th, March, 2010

Page 2: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

00)( 10 ff tiHtiHf eetG

Fermi-Edge Singularity

,2

2

4

ff titG

Sudden change of potentialfelt by the Fermi sea:

At zero temperature in single lead

P. W. Anderson, PRL18, 1049 (1967)

10 HH

Orthogonality Catastrophein quantum point contact:

X-Ray Absorption:

Loop ClosedLineOpen

)()()( fff tGtLtS

Spectrum decomposition:

Page 3: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Scattering Matrix Approach

R

L

ti

ti

R

L

a

a

tS

tBetA

etAtB

b

b

)()(

)()()(

)(

t

dttVt ')'()(10 HH 10 SS Characterize by

000)( )( tif etG

( )i t t ie

t i

Choose with :

20

000)

2)( or,(

22

t

tV

Example: ;01

100

S

0

02

2

1

i

i

e

eS 1ftG ?

But how to connect the Hamiltonians?

Keeling Klich Levitov, PRL97, 116403 (2006)

Page 4: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Map onto Full Counting StatisticsFull Counting Statistics:

SfftG~

1det)( fRft 1det)(

00)(ˆˆ

11 QitiHQitiH

n

nin eeeeeP

00)( 10 tiHti eetG

Fermi-Edge Singularity:

ReT

eTRS

ti

ti

)(

)(~

iiti

itii

LiLi

eABeABe

eABeeAB

eSSeR

22)(

)(22

1

1

RS ~

Let

2

12 RB

2

12 RA

, with

00

01L

Page 5: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Example: Constant Phase Shift (I)

);( ft

otherwise ,0

0 ,)( 0 fttt

T=1 t T=1/2 t

)( ftG

22220

fttttV 0withe.g. Choose Lorentzian Pulses:

FES FCS

)()(0 fttttV dt

dtV

)( )()(0 tttt f

How to represent the delta functionHow to connect and0S 1S

Page 6: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Example: Constant Phase Shift (II)

JZ YS NdA BM, PRB80, 245308 (2009)

When , we have two independent Lorentzian Pulses:

2

0|)1)(1(4

1)(

ii ee

220 4

2 )( ff titG

)()()( 21 fff tGtGtG

)(1 ftG

2

)(t

ft0

ft

Page 7: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Conclusion

How to connect the two Hamiltonian matters

Map FES problem onto FCS

Thank You

Page 8: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

The Effect of Opening & Closing

02

1 RRLLRLLRasym bababiabia00 asym

( ) Imt i

A tt i

Turn on the scattering as

YS JZ NdA BM, PRB 80, 041313 (R) (2009)

tAT 2

Outcome of the wave function:

Optimal Electronic Entangler

Page 9: Fermi-Edge Singularity in Tunnel Junctions Jin Zhang, Y. Sherkunov, N. d’Ambrumenil, B. Muzykantskii University of Warwick, U.K. APS March Meeting, Portland,

Fermi-edge Singularity in 2DEG

D. Cobden, BM, PRL75, 4274 (1995)

xlc HHHH

aaH c

NNc 1lN

..chbaWH x

',

''* 0|)()(|0)(

baWtaWtbtS fffab

Absorption Spectrum:

bbEH ll

aaH c

1NNc 0lN

',

'',

aaVaaH c

1NNc 0lN