Mitigation of $$^{42}$$ 42 Ar/$$^{42}$$ 42 K background for the GERDA Phase II experiment

Abstract Background coming from the $$^{42}$$ 42 Ar decay chain is considered to be one of the most relevant for the Gerda experiment, which searches for the neutrinoless double beta decay of $$^{76}$$ 76 Ge. The sensitivity strongly relies on the absence of background around the Q-value of the deca...

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Bibliographic Details
Main Authors: A. Lubashevskiy, M. Agostini, D. Budjáš, A. Gangapshev, K. Gusev, M. Heisel, A. Klimenko, A. Lazzaro, B. Lehnert, K. Pelczar, S. Schönert, A. Smolnikov, M. Walter, G. Zuzel
Format: Article
Language:English
Published: SpringerOpen 2018-01-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-5499-9
Description
Summary:Abstract Background coming from the $$^{42}$$ 42 Ar decay chain is considered to be one of the most relevant for the Gerda experiment, which searches for the neutrinoless double beta decay of $$^{76}$$ 76 Ge. The sensitivity strongly relies on the absence of background around the Q-value of the decay. Background coming from $$^{42}$$ 42 K, a progeny of $$^{42}$$ 42 Ar, can contribute to that background via electrons from the continuous spectrum with an endpoint at 3.5 MeV. Research and development on the suppression methods targeting this source of background were performed at the low-background test facility LArGe . It was demonstrated that by reducing $$^{42}$$ 42 K ion collection on the surfaces of the broad energy germanium detectors in combination with pulse shape discrimination techniques and an argon scintillation veto, it is possible to suppress $$^{42}$$ 42 K background by three orders of magnitude. This is sufficient for Phase II of the Gerda experiment.
ISSN:1434-6044
1434-6052