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Full Current Statistics in Multiterminal Mesoscopic Conductors

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Presentation on theme: "Full Current Statistics in Multiterminal Mesoscopic Conductors"— Presentation transcript:

1 Full Current Statistics in Multiterminal Mesoscopic Conductors
Dmitry A. Bagrets Universität Karlsruhe Collaboration: Yuli V. Nazarov

2 Outline What is Full Current Statistics? (N-terminal case)
Circuit theory of FCS (non-interacting regime) Master equation approach to FCS (strong Coulomb blockade limit) Weak charge quantization and FCS (weak Coulomb interaction) Conclusions

3 Full Current Statistics
3-terminal case Current conservation number of electrons transferred

4 FCS in N-terminal case Generating function Currents Noise correlations
counting fields Action Probability Currents Noise correlations 3-terminal circuit Higher order correlations

5 Keldysh Method Effective Hamiltonian Generating function
Keldysh path Generating function ( measuring device [spin] ) Conventional Green function technique

6 Circuit Theory Semiclassical approach Boundary conditions
Non-interacting systems Conductance Semiclassical approach Boundary conditions Gauge transform

7 Minimal Action Principal
Total action Action Normalization condition Saddle point ( “1st Kirchhoff’s rule“ ) Matrix current ( “2nd Kirchhoff’s rule“ )

8 Chaotic Quantum Dot Connectors Big current fluctuations! 1-tunnel
2-diffusive 3-ballistic

9 Coulomb Blockade Dot Coulomb blockade system

10 Markov process Master Equation “Orthodox” theory Limits of validity
Rates “Orthodox” theory ( charge quantized ! ) Limits of validity ( No co-tunneling ! )

11 FCS + Master Equation Effective Master equation Generating function
Time arrow Effective Master equation Generating function

12 Coulomb Blockade Dot Big current fluctuations! Coulomb blockade
5 - no interaction

13 Weak Charge Quantization
Panyukov, Zaikin, ’91 Flensberg ’93, Matveev ’95 Nazarov ‘99 Free energy - “Effective” charging energy -Tunnel junctions - Diffusive contacts

14 Coulomb Island - Conductance - Charging energy - Thouless energy
- inverse RC-time Phase Relations between energy scales

15 “Effective” Keldysh Action
Interaction Electrons Electrostatic energy

16 ! Quantum corrections Weak localization correction:
( Random-matrix theory ) Interaction correction Inelastic ( ) Elastic ( ) Divergent ! ? Dissipation!

17 Renormalization Group
“Poor man’s” scaling ( 1-Loop order ) RG Equations “Running” cut-of RG diverges: Metallic saddle point is unstable ! At Charging energy: Equivalence to instanton calculation ! Large phase fluctuations Charge quantization ! [Q,f]=ie

18 Onset of Coulomb Blockade
Critical conductance

19 Full Current Statistics
Connectors 1-tunnel 2-diffusive 3-ballistic

20 Conclusions The theory of FCS in N-terminal circuits:
- Non-interacting regime - Coulomb blockade regime - Weakly interacting regime Evaluation of probability of big current fluctuations Suppression of current fluctuation at Renormalization of transmission eigenvalues Crossover to Coulomb blockade regime at


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