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Final Results of GERDA on the Search for Neutrinoless Double-ß Decay

MPS-Authors
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Bothe,  V.
Division Prof. Dr. James A. Hinton, MPI for Nuclear Physics, Max Planck Society;

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Hakenmüller,  Janina
Division Prof. Dr. Manfred Lindner, MPI for Nuclear Physics, Max Planck Society;

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Hofmann,  W.
Prof. Werner Hofmann, Emeriti, MPI for Nuclear Physics, Max Planck Society;

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Knöpfle,  K. T.
Division Prof. Dr. James A. Hinton, MPI for Nuclear Physics, Max Planck Society;

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Lindner,  M.
Division Prof. Dr. Manfred Lindner, MPI for Nuclear Physics, Max Planck Society;

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Maneschg,  W.
Division Prof. Dr. Manfred Lindner, MPI for Nuclear Physics, Max Planck Society;

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Schreiner,  J.
Division Prof. Dr. Manfred Lindner, MPI for Nuclear Physics, Max Planck Society;

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Schwingenheuer,  B.
Division Prof. Dr. James A. Hinton, MPI for Nuclear Physics, Max Planck Society;

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Simgen,  H.
Division Prof. Dr. Manfred Lindner, MPI for Nuclear Physics, Max Planck Society;

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2009.06079.pdf
(Preprint), 423KB

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Citation

GERDA collaboration, Agostini, M., Araujo, G. R., Bakalyarov, A. M., Balata, M., Barabanov, I., et al. (2020). Final Results of GERDA on the Search for Neutrinoless Double-ß Decay. Physical Review Letters, 125(25): 252502. doi:10.1103/PhysRevLett.125.252502.


Cite as: https://hdl.handle.net/21.11116/0000-0007-99CA-9
Abstract
The GERmanium Detector Array (GERDA) experiment searched for the
lepton-number-violating neutrinoless double-$\beta$ ($0\nu\beta\beta$) decay of
$^{76}$Ge, whose discovery would have far-reaching implications in cosmology
and particle physics. By operating bare germanium diodes, enriched in
$^{76}$Ge, in an active liquid argon shield, GERDA achieved an unprecedently
low background index of $5.2\times10^{-4}$ counts/(keV$\cdot$kg$\cdot$yr) in
the signal region and met the design goal to collect an exposure of 100
kg$\cdot$yr in a background-free regime. When combined with the result of Phase
I, no signal is observed after 127.2 kg$\cdot$yr of total exposure. A limit on
the half-life of $0\nu\beta\beta$ decay in $^{76}$Ge is set at
$T_{1/2}>1.8\times10^{26}$ yr at 90% C.L., which coincides with the sensitivity
assuming no signal.