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 |
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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. |
doi_str_mv | 10.1134/S1062873823705159 |
format | Article |
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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.</description><identifier>ISSN: 1062-8738</identifier><identifier>EISSN: 1934-9432</identifier><identifier>DOI: 10.1134/S1062873823705159</identifier><language>eng</language><publisher>Moscow: Pleiades Publishing</publisher><subject>Cyclotrons ; Distribution functions ; Energy gap ; Fermi liquids ; Hadrons ; Heavy Ions ; Mathematical analysis ; Nuclear Physics ; Physics ; Physics and Astronomy ; Quantum Hall effect</subject><ispartof>Bulletin of the Russian Academy of Sciences. Physics, 2024-02, Vol.88 (2), p.160-164</ispartof><rights>Pleiades Publishing, Ltd. 2024. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2024, Vol. 88, No. 2, pp. 160–164. © Pleiades Publishing, Ltd., 2024.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c1839-32ea60bf02dfcab01f0a41187b5095c3ac1b316ed0c087076aa043d7fe5c2cd93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1134/S1062873823705159$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1134/S1062873823705159$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,41467,42536,51297</link.rule.ids></links><search><creatorcontrib>Vankov, A. B.</creatorcontrib><title>A Migdal Jump in the Quantum Hall Mode</title><title>Bulletin of the Russian Academy of Sciences. Physics</title><addtitle>Bull. Russ. Acad. Sci. Phys</addtitle><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.</description><subject>Cyclotrons</subject><subject>Distribution functions</subject><subject>Energy gap</subject><subject>Fermi liquids</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Mathematical analysis</subject><subject>Nuclear Physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Hall effect</subject><issn>1062-8738</issn><issn>1934-9432</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp1kEFLw0AQhRdRsFZ_gLcFwVt0ZiebzR5LUau0iKjnsNlsakqaxN3m4L93SwUP4mkG3vfeMI-xS4QbREpvXxEykSvKBSmQKPURm6CmNNEpieO4RznZ66fsLIQNgJRayAm7nvFVs65My5_G7cCbju8-HH8ZTbcbt3xh2pav-sqds5PatMFd_Mwpe7-_e5svkuXzw-N8tkws5qQTEs5kUNYgqtqaErAGkyLmqpSgpSVjsSTMXAUWcgUqMwZSqlTtpBW20jRlV4fcwfefowu7YtOPvosnCwJChTL-Fyk8UNb3IXhXF4NvtsZ_FQjFvo7iTx3RIw6eENlu7fxv8v-mb5wuXkI</recordid><startdate>20240201</startdate><enddate>20240201</enddate><creator>Vankov, A. B.</creator><general>Pleiades Publishing</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20240201</creationdate><title>A Migdal Jump in the Quantum Hall Mode</title><author>Vankov, A. B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1839-32ea60bf02dfcab01f0a41187b5095c3ac1b316ed0c087076aa043d7fe5c2cd93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Cyclotrons</topic><topic>Distribution functions</topic><topic>Energy gap</topic><topic>Fermi liquids</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Mathematical analysis</topic><topic>Nuclear Physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Hall effect</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Vankov, A. B.</creatorcontrib><collection>CrossRef</collection><jtitle>Bulletin of the Russian Academy of Sciences. Physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Vankov, A. B.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Migdal Jump in the Quantum Hall Mode</atitle><jtitle>Bulletin of the Russian Academy of Sciences. Physics</jtitle><stitle>Bull. Russ. Acad. Sci. Phys</stitle><date>2024-02-01</date><risdate>2024</risdate><volume>88</volume><issue>2</issue><spage>160</spage><epage>164</epage><pages>160-164</pages><issn>1062-8738</issn><eissn>1934-9432</eissn><abstract>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.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S1062873823705159</doi><tpages>5</tpages></addata></record> |
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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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