Magnetoresistance in the in-plane magnetic field induced semimetallic phase of inverted HgTe quantum wells

被引:3
|
作者
Khouri, T. [1 ,2 ]
Pezzini, S. [1 ,2 ,6 ]
Bendias, M. [3 ]
Leubner, P. [3 ,4 ]
Zeitler, U. [1 ,2 ]
Hussey, N. E. [1 ,2 ]
Buhmann, H. [3 ]
Molenkamp, L. W. [3 ]
Titov, M. [2 ,5 ]
Wiedmann, S. [1 ,2 ]
机构
[1] Radboud Univ Nijmegen, High Field Magnet Lab HFML EMFL, Toernooiveld 7, NL-6525 ED Nijmegen, Netherlands
[2] Radboud Univ Nijmegen, Inst Mol & Mat, Heyendaalseweg 135, NL-6525 AJ Nijmegen, Netherlands
[3] Univ Wurzburg, Phys Inst EP3, D-97074 Wurzburg, Germany
[4] Eindhoven Univ Technol, Dept Appl Phys, NL-5600 MB Eindhoven, Netherlands
[5] ITMO Univ, St Petersburg 197101, Russia
[6] Italian Inst Technol, Ctr Nanotechnol Innovat, NEST, Piazza S Silvestro 12, I-56127 Pisa, Italy
基金
俄罗斯科学基金会;
关键词
GIANT MAGNETORESISTANCE;
D O I
10.1103/PhysRevB.99.075303
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In this study we have measured the magnetoresistance response of inverted HgTe quantum wells in the presence of a large parallel magnetic field up to 33 T. We show that in quantum wells with inverted band structure a monotonically decreasing magnetoresistance is observed when a magnetic field up to the order of 10 T is applied parallel to the quantum well plane. This feature is accompanied by a vanishing of nonlocality and is consistent with a predicted modification of the energy spectrum that becomes gapless at a critical in-plane field B-c. Magnetic fields in excess of B-c allow us to investigate the evolution of the magnetoresistance in this field-induced semimetallic region beyond the known regime. After the longitudinal resistance reaches a minimum in the presumably gapless phase, we observe a strong upturn of the longitudinal resistance. A small residual Hall signal picked up in nonlocal measurements suggests that this feature is likely a bulk phenomenon and is caused by the semimetallicity of the sample. Theoretical calculations indeed support that the origin of these features is classical and a power law upturn of the resistance can be expected due to the specifics of two-carrier transport in thin (semi)metallic samples subjected to large magnetic fields.
引用
收藏
页数:8
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