skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Emergence of superconductivity in topological insulator Bi{sub 2}Se{sub 3} by Sr intercalation

Abstract

Recently superconductivity wasreported by Sr intercalation in topological insulator Bi{sub 2}Se{sub 3}. In this report we extensively study anisotropic superconducting properties of Sr{sub 0.1}Bi{sub 2}Se{sub 3} with transition at ~2.9 through resistivity and DC magnetization measurement. We also discuss synthesis methodology for growth of single crystal Sr-Bi{sub 2}Se{sub 3}. The anisotropic properties of Sr{sub 0.1}Bi{sub 2}Se{sub 3} single crystals were studied using transport measurements. Using Ginzburg Landau formulas the upper critical field H{sub c2}(0) comes out to be 2.1 T and 1.4 T for magnetic field applied along the ab-plane and c-axis of the single crystalsand corresponding Ginzburg - Landau coherence lengths are ξ{sub ab} = 15.3 nm and ξ{sub c} = 10.2 nm. The sample shows weak electronic anisotropy Γ = 1.5. Hall resistivity is linear with field at 10 K.

Authors:
; ;
Publication Date:
OSTI Identifier:
22608862
Resource Type:
Journal Article
Journal Name:
AIP Conference Proceedings
Additional Journal Information:
Journal Volume: 1731; Journal Issue: 1; Conference: DAE solid state physics symposium 2015, Uttar Pradesh (India), 21-25 Dec 2015; Other Information: (c) 2016 Author(s); Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 0094-243X
Country of Publication:
United States
Language:
English
Subject:
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; ANISOTROPY; BISMUTH SELENIDES; CLATHRATES; COHERENCE LENGTH; CRITICAL FIELD; CRYSTAL GROWTH; GINZBURG-LANDAU THEORY; MAGNETIZATION; MONOCRYSTALS; STRONTIUM ADDITIONS; SUPERCONDUCTIVITY; SYNTHESIS; TOPOLOGY

Citation Formats

Shruti,, Maurya, V. K., Srivastava, P., and Patnaik, S., E-mail: spatnaik@mail.jnu.ac.in. Emergence of superconductivity in topological insulator Bi{sub 2}Se{sub 3} by Sr intercalation. United States: N. p., 2016. Web. doi:10.1063/1.4948152.
Shruti,, Maurya, V. K., Srivastava, P., & Patnaik, S., E-mail: spatnaik@mail.jnu.ac.in. Emergence of superconductivity in topological insulator Bi{sub 2}Se{sub 3} by Sr intercalation. United States. https://doi.org/10.1063/1.4948152
Shruti,, Maurya, V. K., Srivastava, P., and Patnaik, S., E-mail: spatnaik@mail.jnu.ac.in. 2016. "Emergence of superconductivity in topological insulator Bi{sub 2}Se{sub 3} by Sr intercalation". United States. https://doi.org/10.1063/1.4948152.
@article{osti_22608862,
title = {Emergence of superconductivity in topological insulator Bi{sub 2}Se{sub 3} by Sr intercalation},
author = {Shruti, and Maurya, V. K. and Srivastava, P. and Patnaik, S., E-mail: spatnaik@mail.jnu.ac.in},
abstractNote = {Recently superconductivity wasreported by Sr intercalation in topological insulator Bi{sub 2}Se{sub 3}. In this report we extensively study anisotropic superconducting properties of Sr{sub 0.1}Bi{sub 2}Se{sub 3} with transition at ~2.9 through resistivity and DC magnetization measurement. We also discuss synthesis methodology for growth of single crystal Sr-Bi{sub 2}Se{sub 3}. The anisotropic properties of Sr{sub 0.1}Bi{sub 2}Se{sub 3} single crystals were studied using transport measurements. Using Ginzburg Landau formulas the upper critical field H{sub c2}(0) comes out to be 2.1 T and 1.4 T for magnetic field applied along the ab-plane and c-axis of the single crystalsand corresponding Ginzburg - Landau coherence lengths are ξ{sub ab} = 15.3 nm and ξ{sub c} = 10.2 nm. The sample shows weak electronic anisotropy Γ = 1.5. Hall resistivity is linear with field at 10 K.},
doi = {10.1063/1.4948152},
url = {https://www.osti.gov/biblio/22608862}, journal = {AIP Conference Proceedings},
issn = {0094-243X},
number = 1,
volume = 1731,
place = {United States},
year = {Mon May 23 00:00:00 EDT 2016},
month = {Mon May 23 00:00:00 EDT 2016}
}