Modeling of GERDA Phase II data

preprint2019arXivOpen access
GERDA collaborationMatteo AgostiniAlexander M. BakalyarovMarco BalataIgor BarabanovLaura BaudisChristian BauerEnrico BellottiSergej BelogurovAlessandro BettiniLeonid BezrukovDariusz BorowiczElisabetta BossioVikas BotheVictor BrudaninRiccardo BrugneraAllen CaldwellCarla CattadoriAndrey ChernogorovTommaso ComellatoValerio D'AndreaElena V. DemidovaNatalia Di MarcoAlexander DomulaEvgenyi DoroshkevichViacheslav EgorovFelix FischerMaria FominaAlbert GangapshevAlberto GarfagniniChris GoochPeter GrabmayrValery GurentsovKonstantin GusevJanina HakenmüllerSabine HemmerRoman HillerWerner HofmannMikael HultLev V. InzhechikJozsef Janicskó CsáthyJosef JochumMatthias JunkerVladimir KazalovYoann KermaïdicThomas KihmIgor V. KirpichnikovAlexander KlimenkoRaphael KneißlKarl T. KnöpfleOleg KochetovVasily N. KornoukhovPatrick KrauseValery V. KuzminovMatthias LaubensteinAndrea LazzaroManfred LindnerIvano LippiAlexey LubashevskiyBayarto LubsandorzhievGuillaume LutterCarla MacolinoBela MajorovitsWerner ManeschgMichael MiloradovicRizalina MingazhevaMarcin MisiaszekPavel MoseevIgor NemchenokKrysztof PanasLuciano PandolaKrysztof PelczarLuigi PertoldiPaolo PiseriAlberto PulliaChloe RansomStefano RiboldiNadezda RumyantsevaCinzia SadaFrancesco SalamidaStefan SchönertJochen SchreinerMario SchüttAnn-Katrin SchützOliver SchulzMario SchwarzBernhard SchwingenheuerOleg SelivanenkoEgor ShevchikMark ShirchenkoHardy SimgenAnatoly SmolnikovDanila StukovLaura VanhoeferAndrey A. VasenkoAnna VeresnikovaChiara VignoliKatharina von SturmThomas WesterChristoph WiesingerMarcin WojcikEvgeny YanovichBirgit ZatschlerIgor ZhitnikovSergey V. ZhukovDaniya ZinatulinaAndreas ZschockeAnna J. ZsigmondKai ZuberGrzegorz Zuzel

Abstract

The GERmanium Detector Array (GERDA) experiment at the Gran Sasso underground laboratory (LNGS) of INFN is searching for neutrinoless double-beta (0νββ0νββ) decay of 76^{76}Ge. 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⋅\cdotyr 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 QββQ_{ββ} for the 0νββ0νββ search, to extract a precise measurement of the half-life of the double-beta decay mode with neutrinos (2νββ2νββ) 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⋅10−3 16.04^{+0.78}_{-0.85} \cdot 10^{-3}\,cts/(kg⋅\cdotkeV⋅\cdotyr) for the enriched BEGe data set and 14.68−0.52+0.47⋅10−3 14.68^{+0.47}_{-0.52} \cdot 10^{-3}\,cts/(kg⋅\cdotkeV⋅\cdotyr) for the enriched coaxial data set. These values are similar to the one of Gerda Phase I despite a much larger number of detectors and hence radioactive hardware components.

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