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Time-dependent transport through a nanostructure coupled to an electromagnetic field in a cavity Viðar Guðmundsson Science Institute, University of Iceland, Iceland [email protected] Berlin, February, 2011 Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 1 / 13

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Page 1: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Time-dependent transport through a nanostructurecoupled to an electromagnetic field in a cavity

Viðar Guðmundsson

Science Institute, University of Iceland, Iceland

[email protected]

Berlin, February, 2011

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 1 / 13

Page 2: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Background - Motivation

PresentlyTime-dependent transport

System - leads, bias

GME many-electron formalism

Coulomb interaction

Finite quantum wire

Quasi-1D leads

Magnetic field

Embedded subsystems

Coulomb blocking, correlations,transients, steady state

FutureExternal photon field

Full EM-coupling

Cavity modes

Polarization

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 2 / 13

Page 3: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Approach

H (t) = He + HCoul︸ ︷︷ ︸diagonalize+cut

+HEM + He−EM

︸ ︷︷ ︸diagonalize+cut→HS

+HL.R + HT(t)

︸ ︷︷ ︸project on system(HS)→GME

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 3 / 13

Page 4: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

e-EM coupling

Full electron-photon coupling∫dr ψ†

{1

2m∗(−i~∇− e

c [A + Aext])2}ψ

=∫

dr ψ†{

12m∗

(−i~∇− e

c A)2}ψ

+ 1c

∫dr j ·Aext + e2

2m∗c

∫dr ρA2

ext

≈∫

dr ψ†{π2

2m∗

}ψ + 1

c

∫dr j ·Aext

= He + He−EM

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 4 / 13

Page 5: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Single cavity mode

HS =∑

aEac†aca + ~νa†a + 1

2∑abcd〈ab|VCoul|cd〉c†ac†bcdcc

+∑ab

c†acb{

gaba + g∗aba†}

HS =∑µ

|µ)Eµ(µ|

+∑µνab|µ)〈µ|V†c†acbV|ν〉(ν|

{gaba + g∗aba†

}

|µ)⊗ |Nph〉 −→ |µ)e−EM︸ ︷︷ ︸diagonalization

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 5 / 13

Page 6: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Energy spectra

x-polarization, B = 0.1 T y-polarization, B = 0.1 T

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 6 / 13

Page 7: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

GME

Weak coupling to leads

Non-Markovian

Memory effects

P = ρLρRTrLR

H lT(t) =

χl(t)∑

q,a

{T l

qad†qlca + (T lqa)∗c†adql

}Reduced statistical operatorρS(t) = P{W (t)}

Liouville-von Neumann equation

W (t) = − i~

[H (t),W (t)] = −iLW (t)

〈A(t)〉 = Tr{W (t)A} = TrS{ρS(t)A}

i~ρS(t) ≈ LSρS(t) + 1i~TrLR

{LT(t)

∫ t

0ds e−i(t−s)L0LT(s)ρLρRρS(s)

}

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 7 / 13

Page 8: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Total charge

x-polarization, B = 0.1 T y-polarization, B = 0.1 T

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 8 / 13

Page 9: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Charge per MES |µ)

x-polarization, B = 0.1 T y-polarization, B = 0.1 T

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 9 / 13

Page 10: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Total number of photons

x-polarization, B = 0.1 T y-polarization, B = 0.1 T

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 10 / 13

Page 11: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Left and Right total current

x-polarization, B = 0.1 T y-polarization, B = 0.1 T

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 11 / 13

Page 12: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Mean total energy

x-polarization, B = 0.1 T y-polarization, B = 0.1 T

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 12 / 13

Page 13: Time-dependent transport through a nanostructure coupled ... · Time-dependenttransportthroughananostructure coupledtoanelectromagneticfieldinacavity ViðarGuðmundsson Science Institute,

Summary

Collaboration with, Andrei Manolescu, Valeriu Moldoveanu,Chi-Shung TangPreliminary results, unpublishedCoulomb InteractionPhoton couplingMany -electron, -photon modelTruncation SchemeExtensive testing needed

New Journal of Physics 11, 073019 (2009), and 113007 (2009)Phys. Rev. B81, 155442 (2010), and 205319 (2010)

Viðar Guðmundsson (RH) t-dependent e-EM transport 2011-02 13 / 13