<p>We report the observation of two distinct thresholds on voltage–current characteristics, accompanied by a peak in broadband current noise occurring between the two threshold voltages, in the insulating state of strongly interacting two-dimensional electron systems. The effects were observed in silicon metal-oxide–semiconductor field-effect transistors and ultra-high mobility SiGe/Si/SiGe heterostructures. A phenomenological theory of the collective depinning of elastic structures can explain the observed results. This provides evidence for the formation of an electron solid in these electron systems and demonstrates the generality of the effect in different classes of two-dimensional electron systems. Interestingly, the double-threshold voltage–current curves, indicative of electron solid formation at low densities, are not observed in the quantum Hall regime. This lack of observation does not confirm the existence of a quasiparticle quantum Hall Wigner solid and indicates that quasiparticles near integer filling do not form an independent subsystem.</p>

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Collective Depinning and Sliding of a Two-Dimensional Quantum Electron Solid in Semiconductors (Brief Review)

  • A. A. Shashkin,
  • S. V. Kravchenko

摘要

We report the observation of two distinct thresholds on voltage–current characteristics, accompanied by a peak in broadband current noise occurring between the two threshold voltages, in the insulating state of strongly interacting two-dimensional electron systems. The effects were observed in silicon metal-oxide–semiconductor field-effect transistors and ultra-high mobility SiGe/Si/SiGe heterostructures. A phenomenological theory of the collective depinning of elastic structures can explain the observed results. This provides evidence for the formation of an electron solid in these electron systems and demonstrates the generality of the effect in different classes of two-dimensional electron systems. Interestingly, the double-threshold voltage–current curves, indicative of electron solid formation at low densities, are not observed in the quantum Hall regime. This lack of observation does not confirm the existence of a quasiparticle quantum Hall Wigner solid and indicates that quasiparticles near integer filling do not form an independent subsystem.