Modeling of Gerda Phase II data
- AGOSTINI M.
- BAKALYAROV A.M.
- BALATA M.
- BARABANOV I.
- BAUDIS L.
- BAUER C.
- BELLOTTI E.
- BELOGUROV S.
- BETTINI A.
- BEZRUKOV L.
- BOROWICZ D.
- BOSSIO E.
- BOTHE V.
- BRUDANIN V.
- BRUGNERA R.
- CALDWELL A.
- CATTADORI C
- CHERNOGOROV A.
- COMELLATO T.
- D'ANDREA V.
- DEMIDOVA E.V.
- DI MARCO N.
- DOMULA A.R.
- DOROSHKEVICH E.
- EGOROV V.
- FISCHER F.
- FOMINA M.
- GANGAPSHEV A.
- GARFAGNINI A.
- GOOCH C.
- GRABMAYR P.
- GURENTSOV V.
- GUSEV K.
- HAKENMÜLLER J.
- HEMMER S.
- HILLER R.
- HOFMANN W.
- HULT MIKAEL
- INZHECHIK L.
- JANICSKO J.
- JOCHUM J.
- JUNKER M.
- KAZALOV V.
- KERMAÏDIC Y.
- KIHM T.
- KIRPICHNIKOV I
- KLIMENKO A.
- KNEISSL R.
- KNOEPFLE K.T.
- KOCHETOV O.
- KORNOUKHOV V.
- KRAUSE P.
- KUZMINOV V.
- LAUBENSTEIN M.
- LAZZARO A.
- LINDNER M.
- LIPPI I.
- LUBASHEVSKY A.
- LUBSANDORZHIEV B.
- LUTTER GUILLAUME
- MACOLINO C.
- MAJOROVITS B.
- MANESCHG W.
- MILORADOVIC M.
- MINGAZHEVA R.
- MISIASZEK M.
- MOSEEV P.
- NEMCHENOK I.
- PANAS K.
- PANDOLA L.
- PELCZAR K.
- PERTOLDI L.
- PISERI P.
- PULLIA A.
- RANSOM C.
- RIBOLDI S.
- RUMYANTSEVA N.
- SADA C.
- SALAMIDA F.
- SCHOENERT S.
- SCHREINER J.
- SCHÜTT M.
- SCHÜTZ A. K.
- SCHULZ O.
- SCHWARZ M.
- SCHWINGENHEUER B.
- SELIVANENKO O.
- SHEVCHIK E.
- SHIRCHENKO M.
- SIMGEN H.
- SMOLNIKOV A.
- STUKOV D.
- VANHOEFER L.
- VASENKO A. A.
- VERESNIKOVA A.
- VIGNOLI C.
- VON STURM K.
- 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.
DOIAbstract
The GERmanium Detector Array (Gerda) experiment at the Gran Sasso underground laboratory (LNGS) of INFN is searching for neutrinoless double-beta (0nbb) 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 Qbb for the 0nbb search, to extract a precise measurement of the half-life of the double-beta decay mode with neutrinos (2nbb) and in order to identify the location of residual impurities. The latter will permit future experiments to build st...
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