Download presentation
Presentation is loading. Please wait.
Published byMagnus Hawkins Modified over 6 years ago
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
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.