The Migdal jump under the quantum Hall regime
- 作者: Vankov A.B.1
-
隶属关系:
- Osipyan Institute of Solid-State Physics of the Russian Academy of Sciences
- 期: 卷 88, 编号 2 (2024)
- 页面: 190-195
- 栏目: New Materials and Technologies for Security Systems
- URL: https://bakhtiniada.ru/0367-6765/article/view/266103
- DOI: https://doi.org/10.31857/S0367676524020048
- EDN: https://elibrary.ru/RTQORV
- ID: 266103
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详细
In two-dimensional electron systems at large values of the Wigner-Seits parameter rs and in the quantum Hall effect mode, the distribution function of particles over Landau levels was calculated. It turned out that at small filling factors, the tail of the distribution function and the magnitude of the Migdal jump are qualitatively different from the case of a Fermi liquid in a zero magnetic field. Due to the presence of the cyclotron energy gap, the Fermi-liquid distortion of the distribution function is significantly suppressed.
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作者简介
A. Vankov
Osipyan Institute of Solid-State Physics of the Russian Academy of Sciences
编辑信件的主要联系方式.
Email: vankov@issp.ac.ru
俄罗斯联邦, Chernogolovka
参考
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