Pulse shape analysis in Gerda Phase II

被引:0
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作者
M. Agostini
G. Araujo
A. M. Bakalyarov
M. Balata
I. Barabanov
L. Baudis
C. Bauer
E. Bellotti
S. Belogurov
A. Bettini
L. Bezrukov
V. Biancacci
E. Bossio
V. Bothe
V. Brudanin
R. Brugnera
A. Caldwell
C. Cattadori
A. Chernogorov
T. Comellato
V. D’Andrea
E. V. Demidova
N. Di Marco
E. Doroshkevich
F. Fischer
M. Fomina
A. Gangapshev
A. Garfagnini
C. Gooch
P. Grabmayr
V. Gurentsov
K. Gusev
J. Hakenmüller
S. Hemmer
R. Hiller
W. Hofmann
J. Huang
M. Hult
L. V. Inzhechik
J. Janicskó Csáthy
J. Jochum
M. Junker
V. Kazalov
Y. Kermaïdic
H. Khushbakht
T. Kihm
K. Kilgus
A. Kirsch
I. V. Kirpichnikov
A. Klimenko
机构
[1] INFN Laboratori Nazionali del Gran Sasso and Gran Sasso Science Institute,Institute of Physics
[2] INFN Laboratori Nazionali del Gran Sasso and Università degli Studi dell’Aquila,Institut für Kern
[3] INFN Laboratori Nazionali del Sud, und Teilchenphysik
[4] Jagiellonian University,Department of Physics and Astronomy
[5] Technische Universität Dresden,Dipartimento di Fisica
[6] Joint Institute for Nuclear Research,Dipartimento di Fisica
[7] European Commission,Institute for Theoretical and Experimental Physics
[8] JRC-Geel,Physik Department
[9] Max-Planck-Institut für Kernphysik,Dipartimento di Fisica e Astronomia
[10] University College London,Physikalisches Institut
[11] Università Milano Bicocca,Physik
[12] INFN Milano Bicocca,Institut
[13] Università degli Studi di Milano and INFN Milano,Institut für Experimentelle Teilchenphysik
[14] Institute for Nuclear Research of the Russian Academy of Sciences,Physik Department
[15] NRC “Kurchatov Institute”,undefined
[16] National Research Centre “Kurchatov Institute”,undefined
[17] Max-Planck-Institut für Physik,undefined
[18] Technische Universität München,undefined
[19] Università degli Studi di Padova,undefined
[20] INFN Padova,undefined
[21] Eberhard Karls Universität Tübingen,undefined
[22] Universität Zürich,undefined
[23] NRNU MEPhI,undefined
[24] Moscow Inst. of Physics and Technology,undefined
[25] Dubna State University,undefined
[26] Karlsruher Institut für Technologie,undefined
[27] Robert Bosch GmbH,undefined
[28] Nuclear Science Division,undefined
[29] Technische Universität München,undefined
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摘要
The GERmanium Detector Array (Gerda) collaboration searched for neutrinoless double-β\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta $$\end{document} decay in 76\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{76}$$\end{document}Ge using isotopically enriched high purity germanium detectors at the Laboratori Nazionali del Gran Sasso of INFN. After Phase I (2011–2013), the experiment benefited from several upgrades, including an additional active veto based on LAr instrumentation and a significant increase of mass by point-contact germanium detectors that improved the half-life sensitivity of Phase II (2015–2019) by an order of magnitude. At the core of the background mitigation strategy, the analysis of the time profile of individual pulses provides a powerful topological discrimination of signal-like and background-like events. Data from regular 228\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{228}$$\end{document}Th calibrations and physics data were both considered in the evaluation of the pulse shape discrimination performance. In this work, we describe the various methods applied to the data collected in Gerda Phase II corresponding to an exposure of 103.7 kg year. These methods suppress the background by a factor of about 5 in the region of interest around Qββ=2039\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q_{\beta \beta }= 2039$$\end{document} keV, while preserving (81±3)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(81\pm 3)$$\end{document}% of the signal. In addition, an exhaustive list of parameters is provided which were used in the final data analysis.
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