Quantum Hall Ferromagnetic-Paramagnetic Transition in p-Si/SiGe/Si Quantum Wells in a Tilted Magnetic Field
Magnetoresistance components ρxx and ρxy were measured in two p-Si/SiGe/Si quantum well samples with an anisotropic g-factor in a tilted magnetic field of up to 18T as a function of temperature (20 mK-2 K) and tilt angle. We analyzed dependences of the conductivity, the activation energy ΔE, and the...
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creator | Drichko, I L Smirnov, I Yu Suslov, A V Mironov, O A Leadley, D R |
description | Magnetoresistance components ρxx and ρxy were measured in two p-Si/SiGe/Si quantum well samples with an anisotropic g-factor in a tilted magnetic field of up to 18T as a function of temperature (20 mK-2 K) and tilt angle. We analyzed dependences of the conductivity, the activation energy ΔE, and the filling factor ν on the tilt angle ⊝. In the sample with density p = 2 × 1011 cm−2 in the vicinity of ν = 2 ΔE(⊝) undergoes a minima at ⊝ ≍ 60o, while ν(⊝) shows a sharp jump. These facts allowed us to conclude that at ⊝ ≍ 60o and ν ≍ 2 a crossing of the Landau levels 0↑ and 1↓ occurs. It leads to the first order ferromagnetic-paramagnetic (F-P) phase transition. A coexistence of two phases at the transition point also supports the idea. However, in another sample, with p = 7.2 × 1010 cm−2, no transition was observed. For both samples we have obtained the dependences of the effective g-factor on the tilt angle, which led us to the conclusion that the F-P transition in the p-Si/SiGe/Si structure in a tilted magnetic field is a result of a violation of the g∗-factor axial symmetry due to disorder. |
doi_str_mv | 10.1088/1742-6596/400/4/042005 |
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We analyzed dependences of the conductivity, the activation energy ΔE, and the filling factor ν on the tilt angle ⊝. In the sample with density p = 2 × 1011 cm−2 in the vicinity of ν = 2 ΔE(⊝) undergoes a minima at ⊝ ≍ 60o, while ν(⊝) shows a sharp jump. These facts allowed us to conclude that at ⊝ ≍ 60o and ν ≍ 2 a crossing of the Landau levels 0↑ and 1↓ occurs. It leads to the first order ferromagnetic-paramagnetic (F-P) phase transition. A coexistence of two phases at the transition point also supports the idea. However, in another sample, with p = 7.2 × 1010 cm−2, no transition was observed. For both samples we have obtained the dependences of the effective g-factor on the tilt angle, which led us to the conclusion that the F-P transition in the p-Si/SiGe/Si structure in a tilted magnetic field is a result of a violation of the g∗-factor axial symmetry due to disorder.</description><identifier>ISSN: 1742-6588</identifier><identifier>EISSN: 1742-6596</identifier><identifier>DOI: 10.1088/1742-6596/400/4/042005</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Camber ; Density ; Ferromagnetism ; Magnetic fields ; Magnetism ; Magnetoresistance ; Magnetoresistivity ; Phase transitions ; Physics ; Quantum wells ; Silicon ; Silicon germanides ; Tilt ; Transition points</subject><ispartof>Journal of physics. 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Conference series</title><description>Magnetoresistance components ρxx and ρxy were measured in two p-Si/SiGe/Si quantum well samples with an anisotropic g-factor in a tilted magnetic field of up to 18T as a function of temperature (20 mK-2 K) and tilt angle. We analyzed dependences of the conductivity, the activation energy ΔE, and the filling factor ν on the tilt angle ⊝. In the sample with density p = 2 × 1011 cm−2 in the vicinity of ν = 2 ΔE(⊝) undergoes a minima at ⊝ ≍ 60o, while ν(⊝) shows a sharp jump. These facts allowed us to conclude that at ⊝ ≍ 60o and ν ≍ 2 a crossing of the Landau levels 0↑ and 1↓ occurs. It leads to the first order ferromagnetic-paramagnetic (F-P) phase transition. A coexistence of two phases at the transition point also supports the idea. However, in another sample, with p = 7.2 × 1010 cm−2, no transition was observed. For both samples we have obtained the dependences of the effective g-factor on the tilt angle, which led us to the conclusion that the F-P transition in the p-Si/SiGe/Si structure in a tilted magnetic field is a result of a violation of the g∗-factor axial symmetry due to disorder.</description><subject>Camber</subject><subject>Density</subject><subject>Ferromagnetism</subject><subject>Magnetic fields</subject><subject>Magnetism</subject><subject>Magnetoresistance</subject><subject>Magnetoresistivity</subject><subject>Phase transitions</subject><subject>Physics</subject><subject>Quantum wells</subject><subject>Silicon</subject><subject>Silicon germanides</subject><subject>Tilt</subject><subject>Transition points</subject><issn>1742-6588</issn><issn>1742-6596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><recordid>eNpdUU1LAzEQDaJgrf4FCXjxsm6-dpM9SrGtUFHpgseQTbKSuh812T34781S24NzmHnDvBmG9wC4xegBIyFSzBlJ8qzIU4ZQylLECELZGZidBucnLMQluAphhxCNwWfg631U3TC2cK2aBi6t932rPjs7OJ28Ka-ODSy96oIbXN9B18F9snXp1q1sTPB44sM2TZimCpauGayBL8ftpbONuQYXtWqCvfmrc1Aun8rFOtm8rp4Xj5tE05wNiamNLkytNUe44oaqTKAIs8zQAptKGISpJYTSvMgoKYRQgvIK1QozUWNN5-D-cHbv--_RhkG2Luj4m-psPwaJuchJVI7zSL37R931o-_ic5JkXJAcUcwiKz-wtO9D8LaWe-9a5X8kRnKyQE7qyklpGS2QTB4soL8J9Xhk</recordid><startdate>20120101</startdate><enddate>20120101</enddate><creator>Drichko, I L</creator><creator>Smirnov, I Yu</creator><creator>Suslov, A V</creator><creator>Mironov, O A</creator><creator>Leadley, D R</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PHGZM</scope><scope>PHGZT</scope><scope>PIMPY</scope><scope>PKEHL</scope><scope>PQEST</scope><scope>PQGLB</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>7U5</scope><scope>8BQ</scope><scope>JG9</scope></search><sort><creationdate>20120101</creationdate><title>Quantum Hall Ferromagnetic-Paramagnetic Transition in p-Si/SiGe/Si Quantum Wells in a Tilted Magnetic Field</title><author>Drichko, I L ; 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Conference series</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Drichko, I L</au><au>Smirnov, I Yu</au><au>Suslov, A V</au><au>Mironov, O A</au><au>Leadley, D R</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Quantum Hall Ferromagnetic-Paramagnetic Transition in p-Si/SiGe/Si Quantum Wells in a Tilted Magnetic Field</atitle><jtitle>Journal of physics. Conference series</jtitle><date>2012-01-01</date><risdate>2012</risdate><volume>400</volume><issue>4</issue><spage>42005</spage><epage>4</epage><pages>42005-4</pages><issn>1742-6588</issn><eissn>1742-6596</eissn><abstract>Magnetoresistance components ρxx and ρxy were measured in two p-Si/SiGe/Si quantum well samples with an anisotropic g-factor in a tilted magnetic field of up to 18T as a function of temperature (20 mK-2 K) and tilt angle. We analyzed dependences of the conductivity, the activation energy ΔE, and the filling factor ν on the tilt angle ⊝. In the sample with density p = 2 × 1011 cm−2 in the vicinity of ν = 2 ΔE(⊝) undergoes a minima at ⊝ ≍ 60o, while ν(⊝) shows a sharp jump. These facts allowed us to conclude that at ⊝ ≍ 60o and ν ≍ 2 a crossing of the Landau levels 0↑ and 1↓ occurs. It leads to the first order ferromagnetic-paramagnetic (F-P) phase transition. A coexistence of two phases at the transition point also supports the idea. However, in another sample, with p = 7.2 × 1010 cm−2, no transition was observed. For both samples we have obtained the dependences of the effective g-factor on the tilt angle, which led us to the conclusion that the F-P transition in the p-Si/SiGe/Si structure in a tilted magnetic field is a result of a violation of the g∗-factor axial symmetry due to disorder.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1742-6596/400/4/042005</doi><tpages>4</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Camber Density Ferromagnetism Magnetic fields Magnetism Magnetoresistance Magnetoresistivity Phase transitions Physics Quantum wells Silicon Silicon germanides Tilt Transition points |
title | Quantum Hall Ferromagnetic-Paramagnetic Transition in p-Si/SiGe/Si Quantum Wells in a Tilted Magnetic Field |
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