Andreev reflection spectroscopy on Bi2X3 (X = Se, Te) topological insulators: Implications for the c-axis superconducting proximity effect
ORAL
Abstract
To understand the superconducting proximity effect that occurs across the c-axis interface of
non-ideal 3D topological insulators, we perform point-contact Andreev reflection (AR) spectroscopy
on Bi2X3 (X=Se,Te) single crystals with Nb tips at 4.2 K. Scanning tunneling spectroscopy is also
used, to locate the Fermi level in the crystals relative to the Dirac point. Robust AR spectra are
observed and analyzed with the Blonder-Tinkham-Klapwijk theory, taking into account tip-induced
spin-orbit coupling, Fermi-surface mismatch, and the co-presence of bulk band states (BBS) and
topological surface states (TSS) at the Fermi level. Spectral analysis using realistic band structures
shows that the superconductivity that can be proximitized into Bi2X3 has a greater non-topological
component than a topological one, since the AR phase space is larger for BBS than for TSS. [1]
[1] C. R. Granstrom et al., https://arxiv.org/abs/1711.00144
non-ideal 3D topological insulators, we perform point-contact Andreev reflection (AR) spectroscopy
on Bi2X3 (X=Se,Te) single crystals with Nb tips at 4.2 K. Scanning tunneling spectroscopy is also
used, to locate the Fermi level in the crystals relative to the Dirac point. Robust AR spectra are
observed and analyzed with the Blonder-Tinkham-Klapwijk theory, taking into account tip-induced
spin-orbit coupling, Fermi-surface mismatch, and the co-presence of bulk band states (BBS) and
topological surface states (TSS) at the Fermi level. Spectral analysis using realistic band structures
shows that the superconductivity that can be proximitized into Bi2X3 has a greater non-topological
component than a topological one, since the AR phase space is larger for BBS than for TSS. [1]
[1] C. R. Granstrom et al., https://arxiv.org/abs/1711.00144
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Presenters
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Chris Granstrom
Univ of Toronto
Authors
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Chris Granstrom
Univ of Toronto
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Igor Fridman
Univ of Toronto
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Hechang Lei
Renmin University, Brookhaven National Laboratory, Brookhaven Natl Lab, Brookhaven National Lab
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Cedomir Petrovic
Brookhaven National Laboratory, Brookhaven Natl Lab, Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA, Brookhaven National Lab
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John Wei
Department of Physics, University of Toronto, Univ of Toronto