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@INPROCEEDINGS{Schfer:1053027,
author = {Schäfer, Christian and Teller, Justus and Bennemann,
Benjamin and Moors, Kristof and Lyatti, Matvey and Lentz,
Florian and Riwar, Roman and Schäpers, Thomas},
title = {{F}rustrated frustration and strong vortex pinning in
{N}b-{P}t-{N}b {J}osephson junction arrays},
reportid = {FZJ-2026-01369},
year = {2025},
abstract = {Josephson junctions are among the most important devices in
quantum computing, ranging from superconducting qubits to
topological protection through Majorana fermions. They are
often studied individually, but arranging them on a one- or
two-dimensional grid to form a Josephson array allows to
leverage collective phenomena. One proposed application is a
topologically protected qubit [1]. When a magnetic field is
applied in the out-of-plane direction, quantized circular
supercurrents known as Josephson vortices appear. An integer
or half-integer number of vortices per unit cell (plaquette)
form a rigid lattice. Because vortex movement produces a
voltage drop across the leads, the DC resistance dips at
(half-)integer values of magnetic flux per unit cell,
creating a "frustration pattern". A promising type of
Josephson junction for Majorana physics is the
multi-terminal Josephson junction, which has more than two
superconducting electrodes. We study the frustration pattern
of a square lattice with in-situ fabricated Nb-Pt-Nb
four-terminal Josephson junctions (4TJJ) and compare it to
arrays of conventionally fabricated two-terminal junctions
(2TJJ) of different sizes. All arrays reproduce the
well-studied frustration behavior. Additionally, the 2TJJ
arrays exhibit a strongly pinned state at low temperatures.
The magnetoresistance of the array is dominated by the
Fraunhofer pattern of the individual junctions. The
four-terminal geometry produces a checkerboard pattern of
alternating fluxes f and f ′ piercing the plaquettes[2].
This type of frustrated frustration manifests as a beating
pattern in the DC resistance. Consequently, 4TJJ arrays
enable us to estimate the spatial extent of the central
weak-link region. This region must be minimized for
topological transitions to occur.[1] Ioffe et al., Nature
415, 503 (2002).[2] Teller et al., Arxiv 2503 14423 (2025)},
month = {Dec},
date = {2025-12-07},
organization = {Workshop on Innovative Nanoscale
Devices and Systems, Waikoloa (USA), 7
Dec 2025 - 12 Dec 2025},
subtyp = {After Call},
cin = {PGI-9 / PGI-10 / HNF / PGI-2},
cid = {I:(DE-Juel1)PGI-9-20110106 / I:(DE-Juel1)PGI-10-20170113 /
I:(DE-Juel1)HNF-20170116 / I:(DE-Juel1)PGI-2-20110106},
pnm = {5222 - Exploratory Qubits (POF4-522) / DFG project
G:(GEPRIS)390534769 - EXC 2004: Materie und Licht für
Quanteninformation (ML4Q) (390534769)},
pid = {G:(DE-HGF)POF4-5222 / G:(GEPRIS)390534769},
typ = {PUB:(DE-HGF)6},
url = {https://juser.fz-juelich.de/record/1053027},
}