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@INPROCEEDINGS{Behner:1053017,
author = {Behner, Gerrit and Jalil, Abdur Rehman and Grützmacher,
Detlev and Schäpers, Thomas},
title = {{S}uperconducting diode effect in {J}osephson junctions
based on topological insulator nanoribbons},
reportid = {FZJ-2026-01361},
year = {2025},
abstract = {Recently, the superconducting diode effect has attracted a
lot of attention [1]. A characteristic of the diode effect
is that the magnitude of the critical supercurrent depends
on the direction in which the current is driven. The
Josephson diode effect occurs when both inversion and
time-reversal symmetry are broken. For Josephson junctions
with a semiconducting [2] or topological insulator [3] weak
link, this can be accomplished by the presence of spin-orbit
coupling in conjunction with an external magnetic field for
the time-reversal symmetry breaking. Recently, the device
layout asymmetry in a multi-terminal Josephson junction also
led to a diode effect, either by keeping one of the
superconducting electrodes floating [4,5] or by phase
biasing the respective junctions [6]. We present
measurements in both two- and multi-terminal Josephson
junctions that clearly demonstrate the Josephson diode
effect and underline the high quality of the devices
fabricated. The fabrication is based on a combination of
selective-area growth of the ternary topological insulator
Bi0.8 Sb1.2 Te3 and shadow mask evaporation of the parent
superconductor Nb. For the multi-terminal junctions we map
out the transport properties as a function of bias currents
and prove the coupling of the junctions by the observation
of the multi-terminal geometry induced Josephson diode
effect. The experimental findings are supported by
simulations based on the resistively and capacitively
shunted junction network model [4]. Regarding the single
junction a pronounced Josephson diode effect is observed
when an in-plane magnetic field is applied perpendicular to
the junction current. Our analysis of the temperature
dependence of the critical current indicates that the
supercurrent is largely carried by topological surface
states which in turn are responsible for the Josephson diode
effect.[1] M. Nadeem, M.S. Fuhrer and X. Wang, Nature
Reviews Physics 10, 558-577 (2023) [2] C. Baumgartner, L.
Fuchs, A. Costa et al., Nature Nanotechnology 1, 39-44
(2022). [3] B. Lu, S. Ikegaya, P. Burset, Y. Tanaka and N.
Nagaosa, Phys. Rev. Lett. 131, 096001 (2023) [4] M. Gupta,
G. Graziano, M. Pendharkar, J. Dong, C. Dempsey, C.
Palmström, V. Pribiag, Nature Communications, 14, 2041-1723
(2023) [5] G. Behner, A. R. Jalil, A. Rupp, H. Lüth, D.
Grützmacher, Th. Schäpers, ACS Nano, accepted, 2025,
arXiv:2410.19311 [6] M. Coraiola, A. Svetogorov, D. Haxell
et al., ACS Nano, 18, 9221-9231 (2024)},
month = {May},
date = {2025-05-06},
organization = {Mallorca Topological Quantum Matter,
Palma de Mallorca (Spain), 6 May 2025 -
9 May 2025},
subtyp = {Invited},
cin = {PGI-9},
cid = {I:(DE-Juel1)PGI-9-20110106},
pnm = {5222 - Exploratory Qubits (POF4-522) / DFG project
G:(GEPRIS)491798118 - Magnetische topologische Isolatoren
für robuste Majorana Zustände (491798118) / DFG project
G:(GEPRIS)390534769 - EXC 2004: Materie und Licht für
Quanteninformation (ML4Q) (390534769)},
pid = {G:(DE-HGF)POF4-5222 / G:(GEPRIS)491798118 /
G:(GEPRIS)390534769},
typ = {PUB:(DE-HGF)6},
url = {https://juser.fz-juelich.de/record/1053017},
}