Abstract

Remnant pockets of carriers left over after formation of a charge density wave (CDW) were brought, by virtue of transverse electric and magnetic fields, to a current-carrying state at quantized Landau Levels. The generated Hall voltage polarizes and puts to sliding the flexible CDW background. The screening from the CDW allows for a so strong redistribution of normal electrons density under the action of the Lorentz force alone, that an integer filling of the lowest Landau level might be reached at one edge at the expense of the full depletion at another edge of the Hall bar. With the Hall field exceeding the sliding threshold, the regime of exactly compensated collective and normal counter-currents develops in the open-circuit direction across the bar. The annihilation of the two currents proceeds via a regular sequence of phase slips which are the space-time vortices of the CDW phase around the enforced amplitude nodes. The resulting spontaneous generation of coherent high (~GHz) frequency signals was detected by observations of multiple Shapiro steps. This picture results from studies of micron-sized Hall bars in crystals of NbSe3 prepared by means of focused ion beams. The interpretation is confirmed and illustrated by a numerical solution of the derived equations. The depinning pulse propagates from edges to the bulk and the sliding sets in, accompanied by the generation of periodic phase slips near the Hall bar edge where the CDW phase is advanced in steps of 2π at expense of the CDW amplitude passing through zero.

Highlights

  • Charge density waves (CDW) are broken-symmetry states ubiquitous in low-dimensional electronic systems

  • The initial motivation of the present studies was to show that the CDW can be driven by the Hall voltage VH originated from the normal current passing in a transverse direction

  • For the bias current I = 10 μA it reaches ~1.5 V/cm which is comparable with the bulk value of the threshold electric field Ext for the onset of the CDW sliding at this temperature.[7]

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Summary

Introduction

Charge density waves (CDW) are broken-symmetry states ubiquitous in low-dimensional electronic systems. We shall show that, thanks to the highly polarizable CDW background, the remnant normal carriers under the quantized magnetic field and the imposed transverse electric current can be put first into the regime of a self-tuned nearly integer quantum Hall (IQH) state.

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Conclusion
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