Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure

Magnetic topological insulator hosts both a non-trivial surface band and quantum anomalous Hall effect when tuning the time reversal symmetry by various chemical doping into the system. Using molecular beam epitaxy, we have synthesized Bi _2−x Cr _x Se _3 /Bi _2 Se _3−y Te _y heterostructure, which...

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Main Authors: Moorthi Kanagaraj, Sun Yizhe, Jiai Ning, Yafei Zhao, Jian Tu, Wenqin Zou, Liang He
Format: Article
Language:English
Published: IOP Publishing 2019-01-01
Series:Materials Research Express
Subjects:
Online Access:https://doi.org/10.1088/2053-1591/ab573f
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author Moorthi Kanagaraj
Sun Yizhe
Jiai Ning
Yafei Zhao
Jian Tu
Wenqin Zou
Liang He
author_facet Moorthi Kanagaraj
Sun Yizhe
Jiai Ning
Yafei Zhao
Jian Tu
Wenqin Zou
Liang He
author_sort Moorthi Kanagaraj
collection DOAJ
description Magnetic topological insulator hosts both a non-trivial surface band and quantum anomalous Hall effect when tuning the time reversal symmetry by various chemical doping into the system. Using molecular beam epitaxy, we have synthesized Bi _2−x Cr _x Se _3 /Bi _2 Se _3−y Te _y heterostructure, which was scrutinized via in situ angle resolved photoemission spectroscopy, ex situ x-ray diffraction, Raman, and x-ray photoemission characteristics analyzing techniques. We used the Hikami-Larkin-Nagaoka formula for quantifying the weak antilocalization limit in Bi _2−x Cr _x Se _3 and Bi _2 Se _3−y Te _y non-magnetic layer coupling near the ferromagnetic transition temperature (∼7 K). A higher concentration of Cr (1.5%) in Bi site leads to bulk carrier density for entire cooling temperature with a bandgap of 85 meV. The proximity effect of Te doped Bi _2 Se _3 with magnetic topological insulator degrades the ferromagnetic response for this heterostructure. Our study suggests that the manipulation of disorder free magnetic top layer and fine tuning of spin–orbit coupling strength in the bottom topological insulator can be helpful to understand the high temperature quantum anomalous Hall effect towards relativistic quantum electronics applications.
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spelling doaj.art-48832c96ab94467db929d0c94548dd362023-08-09T15:22:26ZengIOP PublishingMaterials Research Express2053-15912019-01-017101640110.1088/2053-1591/ab573fTopological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructureMoorthi Kanagaraj0https://orcid.org/0000-0001-7339-714XSun Yizhe1Jiai Ning2Yafei Zhao3Jian Tu4Wenqin Zou5Liang He6School of Electronic Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of ChinaSchool of Electronic Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of ChinaSchool of Electronic Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of ChinaSchool of Electronic Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of ChinaSchool of Electronic Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of ChinaNational Lab of Solid State Microstructures, Department of Physics, Nanjing University , Nanjing 210093, People’s Republic of ChinaSchool of Electronic Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of China; York-Nanjing Joint Center for Spintronics and Nano Engineering (YNJC), School of Electronics Science and Engineering, Nanjing University , Nanjing 210093, People’s Republic of ChinaMagnetic topological insulator hosts both a non-trivial surface band and quantum anomalous Hall effect when tuning the time reversal symmetry by various chemical doping into the system. Using molecular beam epitaxy, we have synthesized Bi _2−x Cr _x Se _3 /Bi _2 Se _3−y Te _y heterostructure, which was scrutinized via in situ angle resolved photoemission spectroscopy, ex situ x-ray diffraction, Raman, and x-ray photoemission characteristics analyzing techniques. We used the Hikami-Larkin-Nagaoka formula for quantifying the weak antilocalization limit in Bi _2−x Cr _x Se _3 and Bi _2 Se _3−y Te _y non-magnetic layer coupling near the ferromagnetic transition temperature (∼7 K). A higher concentration of Cr (1.5%) in Bi site leads to bulk carrier density for entire cooling temperature with a bandgap of 85 meV. The proximity effect of Te doped Bi _2 Se _3 with magnetic topological insulator degrades the ferromagnetic response for this heterostructure. Our study suggests that the manipulation of disorder free magnetic top layer and fine tuning of spin–orbit coupling strength in the bottom topological insulator can be helpful to understand the high temperature quantum anomalous Hall effect towards relativistic quantum electronics applications.https://doi.org/10.1088/2053-1591/ab573fmagnetic topological insulatorepitaxial growthproximity effectquantum anomalous Hall effectweak antilocalization
spellingShingle Moorthi Kanagaraj
Sun Yizhe
Jiai Ning
Yafei Zhao
Jian Tu
Wenqin Zou
Liang He
Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure
Materials Research Express
magnetic topological insulator
epitaxial growth
proximity effect
quantum anomalous Hall effect
weak antilocalization
title Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure
title_full Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure
title_fullStr Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure
title_full_unstemmed Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure
title_short Topological quantum weak antilocalization limit and anomalous Hall effect in semimagnetic Bi2−xCrxSe3/Bi2Se3−yTey heterostructure
title_sort topological quantum weak antilocalization limit and anomalous hall effect in semimagnetic bi2 xcrxse3 bi2se3 ytey heterostructure
topic magnetic topological insulator
epitaxial growth
proximity effect
quantum anomalous Hall effect
weak antilocalization
url https://doi.org/10.1088/2053-1591/ab573f
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