first things first 40 100 24,980. outline physics = surprise physics = surprise electron counting =...
TRANSCRIPT
First things firstFirst things first
40
100
24,980
OutlineOutline
Physics = surprisePhysics = surpriseElectron counting = field theoryElectron counting = field theoryFull Counting Statistic of a scattererFull Counting Statistic of a scattererTwo conductors togetherTwo conductors togetherSaddle pointSaddle pointQuantum effects = Coulomb blockadeQuantum effects = Coulomb blockadeOhmic Renormalization Ohmic Renormalization Quantum renormalizationQuantum renormalization
Full counting statistics of a Full counting statistics of a coherent conductorcoherent conductor
Coherent conductor = scatterer = Coherent conductor = scatterer = {T{Tpp} } (Landauer-Buttiker)(Landauer-Buttiker) Probability to transfer N electrons during time interval Probability to transfer N electrons during time interval t t = =
characteristic function (of characteristic function (of ). ).
Levitov ’93Levitov ’93
Electrons gambleElectrons gamble
1 ( 1) (1 )ln ( ) 2 ln
2 ( 1) (1 )
ip L R
s ip p R L
T e f fdEt
T e f f
( ) exp( ) ( )t tN
i N P N
Charge quantization
L R
Two conductors togetherTwo conductors together
Connect ‘m in seriesConnect ‘m in series
Ohm’s lawOhm’s law
Noises add asNoises add as
FCS?FCS?
A BR R R
2 2
2A A B BS R S R
SR
make a field theorymake a field theory
FixedFixed field(s) in the terminals (Keldysh = field(s) in the terminals (Keldysh = 2)2)
FluctuatingFluctuating field(s) in the node field(s) in the nodeComposition law for the actionComposition law for the action
( ) ( ); ( ) ,2
tet d V t
1 1( ), ( )t t
FCS!!!
Predictions and experimentsPredictions and experiments
Slow realizations, saddle-point solutionSlow realizations, saddle-point solution A-noisy, B- not(environment), shot noise limitA-noisy, B- not(environment), shot noise limit
Beyond noiseBeyond noise Pioneering measurement Pioneering measurement Of the 3Of the 3rdrd cumulant cumulant
M. Kindermann, Yu. V. Nazarov and C. W. J. Beenakker, Phys. Rev. Lett. 90, 246805 (2003).
Reulet B, Senzier J, Prober DE PHYS. REV. LETT. 91, 196601 (2003)
22
4 43 3
4 5
3A A B A
A B AA
QR R RQ Q
R Q R
Properties of the field theoryProperties of the field theory
Low frequencies: always saddle-point solutionLow frequencies: always saddle-point solution Physically: I-V curves, Full Counting StatisticsPhysically: I-V curves, Full Counting Statistics
High frequencies: quantum effects High frequencies: quantum effects Coulomb blockadeCoulomb blockade RRA+BA+B ≠ R ≠ RAA + R + RBB
Renormalization loopRenormalization loop High frequency fluctuations renormalize the properties of low-High frequency fluctuations renormalize the properties of low-
frequency fluctuationsfrequency fluctuations
How big are renormalizations?How big are renormalizations? Universally, GUniversally, GQQ/G /G
2
Q
eG
Coulomb blockade Coulomb blockade (G (G ≪≪GGQQ))
2( )g gC
C VE E N
e 1
2g gNC V
e
Shifts potential= induces charge
CgVg
0
0.1
0.2
0.3
0.4
0.5
0.6
-4 -3 -2 -1 0 1 2 3 4
E
CgVg/e
N
CgVg/e
-4
-2
0
2
4
-4 -3 -2 -1 0 1 2 3 4
Vg
C Cg
N
Where’s the capacitance?Where’s the capacitance?
Never goneNever gone
Defines high-energy cut-offDefines high-energy cut-off
Traditional Coulomb blockade = at the cut-offTraditional Coulomb blockade = at the cut-off
Island
Renormalizations by Ohmic connectorRenormalizations by Ohmic connector
Complicated action – but in terms of Complicated action – but in terms of transmission eigenvaluestransmission eigenvalues
ZGZGQQ – small, but log-divergent at low energies – small, but log-divergent at low energies Program: renormalization of transmission Program: renormalization of transmission
eigenvalues eigenvalues
M. Kindermann and Yu. V. Nazarov, Phys. Rev. Lett. 91, 136802 (2003)
Transmission flowTransmission flow
Key to environmentKey to environment
Consequencies: Consequencies: two classes of coherent conductorstwo classes of coherent conductorsuniversality of resonant tunnelinguniversality of resonant tunneling
(1 )ln Qp
p pZGdT
T Td E
Renormalizations in a quantum dotRenormalizations in a quantum dot
G G ≫≫GGQQ
Is there Coulomb Is there Coulomb blockade?blockade?
Extra parameterExtra parameterSS –mean level –mean level
spacingspacingEECC ≫≫SS
D. A. Bagrets and Yu. V. Nazarov, Phys. Rev. Lett 94, 056801 (2005)
Transmission flowTransmission flow
Very similar, with its own conductanceVery similar, with its own conductance
Conductance itself subject to renormalizationConductance itself subject to renormalization That stops at That stops at
2(1 )
ln k
pp p
k
dTT T
d E T
( / )Th Q SE E G G
Two scenariosTwo scenarios
Blockade with reduced Blockade with reduced Coulomb energyCoulomb energy
Alternative : finite Alternative : finite renormalizationrenormalization