Cyclotron resonance of dirac fermions in InAs/GaSb/InAs quantum wells


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Abstract

The band structure of three-layer symmetric InAs/GaSb/InAs quantum wells confined between AlSb barriers is analyzed theoretically. It is shown that, depending on the thicknesses of the InAs and GaSb layers, a normal band structure, a gapless state with a Dirac cone at the center of the Brillouin zone, or inverted band structure (two-dimensional topological insulator) can be realized in this system. Measurements of the cyclotron resonance in structures with gapless band spectra carried out for different electron concentrations confirm the existence of massless Dirac fermions in InAs/GaSb/InAs quantum wells.

About the authors

S. S. Krishtopenko

Institute for Physics of Microstructures; Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950; Montpellier, 34095

A. V. Ikonnikov

Institute for Physics of Microstructures; Lobachevsky State University of Nizhny Novgorod

Author for correspondence.
Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950; Nizhny Novgorod, 603950

K. V. Maremyanin

Institute for Physics of Microstructures; Lobachevsky State University of Nizhny Novgorod

Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950; Nizhny Novgorod, 603950

L. S. Bovkun

Institute for Physics of Microstructures

Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950

K. E. Spirin

Institute for Physics of Microstructures

Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950

A. M. Kadykov

Institute for Physics of Microstructures; Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950; Montpellier, 34095

M. Marcinkiewicz

Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
France, Montpellier, 34095

S. Ruffenach

Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
France, Montpellier, 34095

C. Consejo

Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
France, Montpellier, 34095

F. Teppe

Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
France, Montpellier, 34095

W. Knap

Laboratoire Charles Coulomb (L2C), UMR CNRS 5221

Email: antikon@ipmras.ru
France, Montpellier, 34095

B. R. Semyagin

Rzhanov Institute of Semiconductor Physics, Siberian Branch

Email: antikon@ipmras.ru
Russian Federation, Novosibirsk, 630090

M. A. Putyato

Rzhanov Institute of Semiconductor Physics, Siberian Branch

Email: antikon@ipmras.ru
Russian Federation, Novosibirsk, 630090

E. A. Emelyanov

Rzhanov Institute of Semiconductor Physics, Siberian Branch

Email: antikon@ipmras.ru
Russian Federation, Novosibirsk, 630090

V. V. Preobrazhenskii

Rzhanov Institute of Semiconductor Physics, Siberian Branch

Email: antikon@ipmras.ru
Russian Federation, Novosibirsk, 630090

V. I. Gavrilenko

Institute for Physics of Microstructures; Lobachevsky State University of Nizhny Novgorod

Email: antikon@ipmras.ru
Russian Federation, Nizhny Novgorod, 603950; Nizhny Novgorod, 603950


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