quantum impurities out of equilibrium: (bethe ansatz for open systems)
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Dresden, April 2006. Quantum Impurities out of equilibrium: (Bethe Ansatz for open systems). Pankaj Mehta & N.A. Outline. Non-equilibrium Dilemmas. Nonequilibrium systems are relatively poorly understood compared to their equilibrium counterpart. - PowerPoint PPT PresentationTRANSCRIPT
Quantum Impurities out of equilibrium:(Bethe Ansatz for open systems)
Dresden, April 2006
Pankaj Mehta & N.A.
Outline
Non-equilibrium Dilemmas
● Many of our standard physical ideas and concepts are not applicable
● No unifying theory such as Boltzman's statistical mechanics
● Non-equilibrium systems are all different- it is unclear what if anything they all have in common.
● Nonequilibrium systems are relatively poorly understood compared to their equilibrium counterpart.
● Interplay between non-equilibrium dynamics and strong correlations
Non-equilibrium Dilemmas
● Nonequilibrium physics is difficult and compared with equilibrium physics is poorly understood
● Many of our standard physical ideas and concepts are not applicable
● No unifying theory such as Bolzman's statistical mechanics
● Non-equilibrium systems are all different- it is unclear what if anything they all have in common.
● Interplay of non-equilibrium and strong correlations
● Non-equilibrium Steady-State● Quantum Impurities
Study simplest systems:
Kondo Impurities – Strong Correlations out of Equilibrium
Inoshita:Science 24 July 1998: Vol. 281. no. 5376, pp. 526 - 527
● Can control the number of electrons on the dot using gate voltage ● For odd number of electrons- quantum dot acts like a quantum impurity (Kondo, Interacting Resonant Level Model)●Quantum impurity models exhibit new collective behaviors such as the Kondo effect
Quantum Impurities out of Equilibrium
Strong Correlations =New Collective Behavior (eg Kondo Effect)
=
No Minimization Principle No Scaling/ RG No simple intuition
Nonequilibrium Dynamics =
No valid perturbation theory Need new degrees of freedom
Need new conceptual and theoretical tools!
Quantum Impurities out of Equilibrium
Non-equilibrium: Time-dependent Description
The Steady State
Non-equilibrium: Time-independent Description
Scattering States (QM)
● Scattering by a localized potential is given by the Lippman-Schwinger equation:
● Since we are in a steady-state, can go to a time-independent picture.
The Scattering state (Many body)
A scattering eigenstate is determined by its incoming asymptotics: the baths
The wave-function schematically: (the outgoing asymptotics needs to be solved)
Must carry out construction for a strongly correlated system.
The Scattering State (Many body)
1
To construct the nonequilibrium scattering state, it is useful to unfold the leadsso that there are only right-movers:
The scattering eigenstate determined by N1 incoming electrons in lead 1, and N2 electrons in lead 2 (determined by and )
The Scattering Bethe-Ansatz
.
.
IRL: The Scattering State I
.
IRL: The Scattering State II
.
The Scattering State III
.
Bethe Anstaz basis vs. Fock basis
Fock Basis Bethe-Ansatz Basis
● Energy levels are infinitely degenerate (linear spectrum) ● Once again the momentum are not specified - need choose basis● We must choose the momenta of the incoming particles to look like two free Fermi seas
Fermi – Dirac distribution
Bethe –Ansatz distribution
S=1 S≠1
Basis
Fermi-seaMomenta
S-Matrix
IRL: Current & Dot Occupation IRL: Current & Dot Occupation
IRL: Current vs. Voltage
● Exact current as a function of Voltage numerically
● Notice the current is non-monotonic in U, with duality between small and large U● Scaling - out of equilibrium● Can easily generalize to finite temperature
IRL: Current vs. Voltage● Exact current as a function of Voltage:
● Notice the current is non-monotonic in U, with duality between small and large U● Can easily generalize to finite temperature case
GENERAL FRAMEWORK TO CALCULATE STEADY-STATE QUANTITIES EXACTLY!
IRL: Current vs. Voltage
Kondo: The Current (in progress) Must solve BA equations:
In continuum version (Wiener-Hopf):
Kondo: The Current (in progress)
The Current:
Evaluated in the scattering state:
Conclusions