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Modeling of GERDA Phase II Data

Agostini M.,Bakalyarov A. M.,Balata M.,Barabanov I.,Baudis L.,Bauer C., INFN Milano Bicocca, NRNU MEPhI, INFN Padova,Bezrukov L.,Borowicz D.,Bossio E.,Bothe V.,Brudanin V.,Caldwell A.,Cattadori C., National Research Centre “Kurchatov Institute”,Comellato T.,D’Andrea V.,Demidova E. V.,Di Marco N.,Domula A.,Doroshkevich E.,Egorov V.,Fischer F.,Fomina M., Max-Planck-Institut für Kernphysik,Gooch C.,Grabmayr P.,Gurentsov V., Technische Universität München,Hakenmüller J.,Hemmer S.,Hiller R.,Hofmann W.,Hult M., Moscow Inst. of Physics and Technology, Leibniz-Institut für Kristallzüchtung,Jochum J.,Junker M.,Kazalov V.,Kermaïdic Y.,Kihm T.,Kirpichnikov I. V., Dubna State University,Kneißl R.,Knöpfle K. T.,Kochetov O., Institute for Nuclear Research of the Russian Academy of Sciences,Krause P.,Kuzminov V. V.,Laubenstein M.,Lazzaro A.,Lindner M.,Lippi I.,Lubashevskiy A.,Lubsandorzhiev B.,Lutter G., LAL, CNRSIN2P, Université Paris-Saclay,Majorovits B.,Maneschg W.,Miloradovic M.,Mingazheva R.,Misiaszek M.,Moseev P.,Panas K., Pandola L.,Pelczar K.,Piseri P.,Pullia A.,Ransom C.,Riboldi S., Joint Institute for Nuclear Research,Salamida F.,Schönert S.,Schreiner J.,Schütt M.,Schütz A-K.,Schulz O.,Schwarz M.,Schwingenheuer B.,Selivanenko O.,Shevchik E.,Shirchenko M.,Simgen H.,Stukov D.,Vanhoefer L.,Vasenko A. A.,Veresnikova A.,Vignoli C.,Wester T.,Wiesinger C.,Wojcik M.,Yanovich E.,Zatschler B.,Zhitnikov I.,Zhukov S. V.,Zinatulina D.,Zschocke A.,Zsigmond A. J.,Zuber K.,Zuzel G.

˜The œJournal of high energy physics/˜The œjournal of high energy physics(2020)

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摘要
The GERmanium Detector Array (Gerda) experiment at the Gran Sasso underground laboratory (LNGS) of INFN is searching for neutrinoless double-beta (0νββ) decay of 76Ge. The technological challenge of Gerda is to operate in a “background-free” regime in the region of interest (ROI) after analysis cuts for the full 100 kg·yr target exposure of the experiment. A careful modeling and decomposition of the full-range energy spectrum is essential to predict the shape and composition of events in the ROI around Qββ for the 0νββ search, to extract a precise measurement of the half-life of the double-beta decay mode with neutrinos (2νββ) and in order to identify the location of residual impurities. The latter will permit future experiments to build strategies in order to further lower the background and achieve even better sensitivities. In this article the background decomposition prior to analysis cuts is presented for Gerda Phase II. The background model fit yields a flat spectrum in the ROI with a background index (BI) of $$ {16.04}_{-0.85}^{+0.78}\cdotp {10}^{-3} $$ cts/(keV·kg·yr) for the enriched BEGe data set and $$ {14.68}_{-0.52}^{+0.47}\cdotp {10}^{-3} $$ cts/(keV·kg·yr) for the enriched coaxial data set. These values are similar to the one of Phase I despite a much larger number of detectors and hence radioactive hardware components.
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Dark Matter and Double Beta Decay (experiments)
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