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Transition between electron localization and antilocalization in graphene.

F V Tikhonenko1, A A Kozikov, A K Savchenko

  • 1School of Physics, University of Exeter, EX4 4QL Exeter, United Kingdom.

Physical Review Letters
|April 7, 2010
PubMed
Summary
This summary is machine-generated.

Quantum interference in graphene causes antilocalization, observed as negative magnetoconductance. This effect transitions with carrier density and temperature, persisting up to 200 K due to weak electron-phonon scattering.

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Area of Science:

  • Condensed matter physics
  • Quantum mechanics
  • Materials science

Background:

  • Quantum interference significantly impacts charge carrier behavior in materials.
  • Understanding electron transport in graphene is crucial for next-generation electronics.
  • Localization and antilocalization phenomena are key to characterizing quantum transport.

Purpose of the Study:

  • To investigate quantum interference effects on charge carriers in graphene.
  • To identify conditions leading to weak localization versus antilocalization.
  • To determine the temperature stability of quantum interference in graphene.

Main Methods:

  • Experimental measurement of conductance in graphene.
  • Application of magnetic fields to observe magnetoconductance.
  • Systematic variation of carrier density and temperature.

Main Results:

  • Quantum interference in graphene leads to antilocalization, evidenced by negative magnetoconductance.
  • Both weak localization and antilocalization were observed, tunable by experimental conditions.
  • A transition from localization to antilocalization occurs with decreased carrier density and increased temperature.
  • Quantum interference effects were observed to persist up to approximately 200 K.

Conclusions:

  • Quantum interference in graphene exhibits tunable localization and antilocalization behaviors.
  • Carrier density and temperature are critical parameters controlling the transition between localization regimes.
  • Weak electron-phonon scattering allows quantum interference phenomena in graphene to survive at high temperatures.