Coulomb drag in graphene Igor Gornyi Karlsruhe Institute of - - PowerPoint PPT Presentation

coulomb drag in graphene
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Coulomb drag in graphene Igor Gornyi Karlsruhe Institute of - - PowerPoint PPT Presentation

Coulomb drag in graphene Igor Gornyi Karlsruhe Institute of Technology Collaboration: Mikhail Titov (Nijmegen) Boris Narozhny (Karlsruhe) Pavel Ostrovsky (Stuttgart) Michael Schtt (Karlsruhe) Alexander Mirlin (Karlsruhe) Phys. Rev. B 85 ,


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Igor Gornyi

Karlsruhe Institute of Technology

Collaboration:

Mikhail Titov (Nijmegen) Boris Narozhny (Karlsruhe) Pavel Ostrovsky (Stuttgart) Michael Schütt (Karlsruhe) Alexander Mirlin (Karlsruhe)

  • Phys. Rev. B 85, 195421 (2012)

+ arXiv:1205.5018

Coulomb drag in graphene

Chernogolovka, 14 September 2012

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What is Coulomb drag?

Coulomb drag = response of the passive layer to a current in the active layer mediated by Coulomb interaction

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Coulomb drag measurements

Gramila, Eisenstein, MacDonald et.al ., Phys. Rev. Lett. 66, 1216 (1991)

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Theory: 2D

Pogrebinskii (1977) – introduced Coulomb drag Zheng, MacDonald (1993) – memory function Jauho, Smith (1993) – kinetic equation Kamenev, Oreg (1995) – diagrammatics Flensberg et al. (1995) – diagrammatics ...

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Coulomb drag: why interesting?

  • no drag without interaction:

probe of inter-electron correlations

  • provides information about inelastic processes,

phase-coherent phenomena

  • drag is related to particle-hole asymmetry

Drag in graphene near the Dirac point ?

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Particle-hole asymmetry

Example: strong magnetic field (i) Curvature  normal positive drag (ii) Landau levels DoS  anomalous oscillatory drag IG, Mirlin, von Oppen (2004)

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Drag in 2D: standard theory

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Drag in graphene

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Dirac spectrum at low energies electron-hole symmetry at the Dirac point linear spectrum – no Galilean invariance

non-trivial single-layer conductivity

small interlayer distance d

News in graphene

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Drag in graphene: experiment

single-gate device

Kim, Jo, Nah, Yao, Banerjee, and Tutuc, Phys. Rev. B 83, 161401 (2011)

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Drag in graphene: experiment

single-gate device

Kim, Jo, Nah, Yao, Banerjee, and Tutuc, Phys. Rev. B 83, 161401 (2011)

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Drag in graphene: experiment

double-gate device

Tutuc and Kim, Solid State Comm. (2012)

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Drag in graphene: experiment

double-gate device

Tutuc and Kim, Solid State Comm. (2012)

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“clean” substrate and spacer – BN

smaller inter-layer spacing d = 1-10 nm

Drag in graphene: experiment

  • Double-gate setup:

Gorbachev, Geim, Novoselov, Ponomarenko et al. ArXiv:1206.6626

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double-gate device

Gorbachev, Geim, Novoselov, Ponomarenko et al. ArXiv:1206.6626

Drag in graphene: experiment

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double-gate device

Drag in graphene: experiment

Gorbachev, Geim, Novoselov, Ponomarenko et al. ArXiv:1206.6626

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double-gate device

Drag in graphene: experiment

Gorbachev, Geim, Novoselov, Ponomarenko et al. ArXiv:1206.6626

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disordered graphene

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Second-order perturbation theory

non-linear susceptibility (rectification function) screened interlayer interaction

Narozhny, Titov, IG, and Ostrovsky, PRB (2012)

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arbitrary values of chemical potential controlled perturbation theory

weak interaction static screening is sufficient

dominant scattering mechanism is due to disorder

– qualitatively not important:

  • plasmons
  • spectrum renormalization
  • energy dependence of disorder

scattering time

non-degenerate relativistic gas Fermi liquid

experimental condition

Drag in disordered graphene

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comparison with experiment

courtesy of L. Ponomarenko

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ultra-clean graphene

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Graphene: no Galilean invariance, relativistic dynamics

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Clean vs. disordered graphene

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Kinetic theory of the drag

Linearized kinetic equation:

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Inelastic scattering in graphene

Linear spectrum:

Velocity is not equivalent to momentum: momentum conservation does not prevent current relaxation

  • Finite transport rate due to inelastic e-e scattering

Collinear scattering singularity: momentum conservation = energy conservation

  • Fast thermalization within a given direction

Kashuba '08, Fritz, Müller, Schmalian, Sachdev '08

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Collinear scattering singularity

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Double-layer graphene

Only two modes (velocity and momentum) in each layer: Fast unidirectional thermalization between layers: Kinetic (integral) equation reduces to a 3x3 matrix equation! Hydrodynamics: total momentum + particle currents

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Hydrodynamic equations

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Scattering rates: Golden Rule

close to the Dirac point away from the Dirac point

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Drag resistivity

Equal layers: Non-equal layers near the Dirac point

Finite drag at the Dirac point in the clean case!

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neutrality point

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Drag rate: beyond Golden Rule

Exactly at the Dirac point: finite third-order drag

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Diffusive regime

Conventional (second-order) drag vanishes at the Dirac point Third-order (Levchenko & Kamenev 2008) drag dominates

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Correlated disorder

Ballistic regime: Diffusive regime: interlayer Cooper mode (IG, Yashenkin, Khveshchenko '99)

Correlated elastic scattering in the two layers with common impurities

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Correlated disorder

Correlated elastic scattering in the two layers with common impurities Moderately correlated disorder:

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2nd vs. 3rd order drag

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Drag at the Dirac point

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Magnetodrag

Gorbachev, Geim, Novoselov, Ponomarenko et al. ArXiv:1206.6626

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Summary

Coulomb drag in graphene:

  • Perturbation theory
  • Kinetic theory (3 mode hydrodynamics)
  • Clean graphene (equilibrated drag)
  • Peak at the Dirac point

3rd order drag, drag with correlated disorder