“Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures

We show that in dilute metallic p-SiGe heterostructures, magnetic field can cause multiple quantum Hall-insulator-quantum Hall transitions. The insulating states are observed between quantum Hall states with filling factors = 1 and 2 and, for the first time, between = 2 and 3 and between = 4 and 6....

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Online Access:http://hdl.handle.net/2047/d20000354
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spelling ndltd-NEU--neu-3310242016-04-25T16:14:18Z“Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructuresWe show that in dilute metallic p-SiGe heterostructures, magnetic field can cause multiple quantum Hall-insulator-quantum Hall transitions. The insulating states are observed between quantum Hall states with filling factors = 1 and 2 and, for the first time, between = 2 and 3 and between = 4 and 6. The latter are in contradiction with the original global phase diagram for the quantum Hall effect. We suggest that the application of a (perpendicular) magnetic field induces insulating behaviour in metallic p-SiGe heterostructures in the same way as in Si MOSFETs. This insulator is then in competition with, and interrupted by, integer quantum Hall states leading to the multiple re-entrant transitions. The phase diagram which accounts for these transition is similar to that previously obtained in Si MOSFETs thus confirming its universal character.http://hdl.handle.net/2047/d20000354
collection NDLTD
sources NDLTD
description We show that in dilute metallic p-SiGe heterostructures, magnetic field can cause multiple quantum Hall-insulator-quantum Hall transitions. The insulating states are observed between quantum Hall states with filling factors = 1 and 2 and, for the first time, between = 2 and 3 and between = 4 and 6. The latter are in contradiction with the original global phase diagram for the quantum Hall effect. We suggest that the application of a (perpendicular) magnetic field induces insulating behaviour in metallic p-SiGe heterostructures in the same way as in Si MOSFETs. This insulator is then in competition with, and interrupted by, integer quantum Hall states leading to the multiple re-entrant transitions. The phase diagram which accounts for these transition is similar to that previously obtained in Si MOSFETs thus confirming its universal character.
title “Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures
spellingShingle “Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures
title_short “Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures
title_full “Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures
title_fullStr “Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures
title_full_unstemmed “Forbidden” transitions between quantum Hall and insulating phases in p-SiGe heterostructures
title_sort “forbidden” transitions between quantum hall and insulating phases in p-sige heterostructures
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url http://hdl.handle.net/2047/d20000354
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