A Migdal Jump in the Quantum Hall Mode

The distribution function of particles over Landau levels is calculated in two-dimensional electron systems at high values of Wigner–Seits parameter r s and in the mode of the quantum Hall effect. At low filling factors, the tail of the distribution function and the magnitude of the Migdal jump diff...

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Veröffentlicht in:Bulletin of the Russian Academy of Sciences. Physics 2024-02, Vol.88 (2), p.160-164
1. Verfasser: Vankov, A. B.
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description The distribution function of particles over Landau levels is calculated in two-dimensional electron systems at high values of Wigner–Seits parameter r s and in the mode of the quantum Hall effect. At low filling factors, the tail of the distribution function and the magnitude of the Migdal jump differ qualitatively from a Fermi liquid in a zero magnetic field. The Fermi-liquid distortion of the distribution function is strongly suppressed by the existence of a cyclotron energy gap.
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B.</creator><creatorcontrib>Vankov, A. B.</creatorcontrib><description>The distribution function of particles over Landau levels is calculated in two-dimensional electron systems at high values of Wigner–Seits parameter r s and in the mode of the quantum Hall effect. At low filling factors, the tail of the distribution function and the magnitude of the Migdal jump differ qualitatively from a Fermi liquid in a zero magnetic field. 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subjects Cyclotrons
Distribution functions
Energy gap
Fermi liquids
Hadrons
Heavy Ions
Mathematical analysis
Nuclear Physics
Physics
Physics and Astronomy
Quantum Hall effect
title A Migdal Jump in the Quantum Hall Mode
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