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The GERmanium Detector Array (Gerda) collaboration searched for neutrinoless double-β decay in 76Ge 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 228Th 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 keV, while preserving (81±3)% of the signal. In addition, an exhaustive list of parameters is provided which were used in the final data analysis.

A bstract The Borexino detector measures solar neutrino fluxes via neutrino-electron elastic scattering. Observed spectra are determined by the solar- ν e survival probability P ee ( E ), and the chiral couplings of the neutrino and electron. Some theories of physics beyond the Standard Model postulate the existence of Non-Standard Interactions (NSI’s) which modify the chiral couplings and P ee ( E ). In this paper, we search for such NSI’s, in particular, flavor-diagonal neutral current interactions that modify the ν e e and ν τ e couplings using Borexino Phase II data. Standard Solar Model predictions of the solar neutrino fluxes for both high- and low-metallicity assumptions are considered. No indication of new physics is found at the level of sensitivity of the detector and constraints on the parameters of the NSI’s are placed. In addition, with the same dataset the value of sin 2 θ W is obtained with a precision comparable to that achieved in reactor antineutrino experiments .

The beta decay of$$^{77}$$77 Ge and$$^{77\\textrm{m}}$$77 m Ge, both produced by neutron capture on$$^{76}$$76 Ge, is a potential background for Germanium based neutrinoless double-beta decay search experiments such as GERDA or the LEGEND experiment. In this work we present a search for$$^{77}$$77 Ge decays in the full GERDA Phase II data set. A delayed coincidence method was employed to identify the decay of$$^{77}$$77 Ge via the isomeric state of$$^{77}$$77 As ($$9/2^+$$9 / 2 + ,$${475}\\,\\hbox {keV}$$475 keV ,$${T_{1/2} = {114}\\,{\\upmu }\\hbox {s}}$$T 1 / 2 = 114 μ s ,$$^{77\\textrm{m}}$$77 m As). New digital signal processing methods were employed to select and analyze pile-up signals. No signal was observed, and an upper limit on the production rate of$$^{77}$$77 Ge was set at$$<0.216$$< 0.216 nuc/(kg$$\\cdot $$· yr) (90% CL). This corresponds to a total production rate of$$^{77}$$77 Ge and$$^{77\\textrm{m}}$$77 m Ge of$$<{0.38}$$< 0.38 nuc/(kg$$\\cdot $$·  yr) (90% CL), assuming equal production rates. A previous Monte Carlo study predicted a value for in-situ$$^{77}$$77 Ge and$$^{77\\textrm{m}}$$77 m Ge production of (0.21 ± 0.07) nuc/(kg.yr), a prediction that is now further corroborated by our experimental limit. Moreover, tagging the isomeric state of$$^{77\\textrm{m}}$$77 m As can be utilised to further suppress the$$^{77}$$77 Ge background. Considering the similar experimental configurations of LEGEND-1000 and GERDA, the cosmogenic background in LEGEND-1000 at LNGS is estimated to remain at a sub-dominant level.

A search for full energy depositions from bosonic keV-scale dark matter candidates of masses between 65 and 1021 keV has been performed with data collected during Phase II of the GERmanium Detector Array ( Gerda ) experiment. Our analysis includes direct dark matter absorption as well as dark Compton scattering. With a total exposure of 105.5 kg years, no evidence for a signal above the background has been observed. The resulting exclusion limits deduced with either Bayesian or Frequentist statistics are the most stringent direct constraints in the major part of the 140–1021 keV mass range. As an example, at a mass of 150 keV the dimensionless coupling of dark photons and axion-like particles to electrons has been constrained to α ′ / α < 8.7 × 10 - 24 and g ae < 3.3 × 10 - 12 at 90% credible interval (CI), respectively. Additionally, a search for peak-like signals from beyond the Standard Model decays of nucleons and electrons is performed. We find for the inclusive decay of a single neutron in 76 Ge a lower lifetime limit of τ n > 1.5 × 10 24 years and for a proton τ p > 1.3 × 10 24 years at 90% CI. For the electron decay e - → ν e γ a lower limit of τ e > 5.4 × 10 25 years at 90% CI has been determined.

The radioactive isotope 85 Kr is found in significant quantities in the atmosphere largely due to nuclear industry. Its β -decay with a half-life of 10.7 years and a Q-value of 687 keV is a dangerous background source for low-threshold noble gas and liquid detectors, which distill their detector medium from air. The Gerda experiment was operating high-purity germanium detectors immersed in a clean liquid argon bath deep underground to search for neutrinoless double beta decay with unprecedented sensitivity. The 85 Kr specific activity in the liquid argon at the start of the second phase of the experiment has been determined to be ( 0.36 ± 0.03 )  mBq/kg through an analysis of the full subsequent data set that exploits the excellent γ -ray spectroscopic capabilities of Gerda .

We search for tri-nucleon decays of$$^{76}$$76 Ge in the dataset from the GERmanium Detector Array (GERDA) experiment. Decays that populate excited levels of the daughter nucleus above the threshold for particle emission lead to disintegration and are not considered. The ppp-, ppn-, and pnn-decays lead to$$^{73}$$73 Cu,$$^{73}$$73 Zn, and$$^{73}$$73 Ga nuclei, respectively. These nuclei are unstable and eventually proceed by the beta decay of$$^{73}$$73 Ga to$$^{73}$$73 Ge (stable). We search for the$$^{73}$$73 Ga decay exploiting the fact that it dominantly populates the 66.7 keV$$^{73m}$$73 m Ga state with half-life of 0.5 s. The nnn-decays of$$^{76}$$76 Ge that proceed via$$^{73m}$$73 m Ge are also included in our analysis. We find no signal candidate and place a limit on the sum of the decay widths of the inclusive tri-nucleon decays that corresponds to a lower lifetime limit of 1.2$$\\times $$× 10$$^{26}$$26  yr  (90% credible interval). This result improves previous limits for tri-nucleon decays by one to three orders of magnitude.

The ability to detect liquid argon scintillation light from within a densely packed high-purity germanium detector array allowed the Gerda experiment to reach an exceptionally low background rate in the search for neutrinoless double beta decay of 76 Ge. Proper modeling of the light propagation throughout the experimental setup, from any origin in the liquid argon volume to its eventual detection by the novel light read-out system, provides insight into the rejection capability and is a necessary ingredient to obtain robust background predictions. In this paper, we present a model of the Gerda liquid argon veto, as obtained by Monte Carlo simulations and constrained by calibration data, and highlight its application for background decomposition.

The radioactive isotope Kr is found in significant quantities in the atmosphere largely due to nuclear industry. Its -decay with a half-life of 10.7 years and a Q-value of 687 keV is a dangerous background source for low-threshold noble gas and liquid detectors, which distill their detector medium from air. The Gerda experiment was operating high-purity germanium detectors immersed in a clean liquid argon bath deep underground to search for neutrinoless double beta decay with unprecedented sensitivity. The Kr specific activity in the liquid argon at the start of the second phase of the experiment has been determined to be  mBq/kg through an analysis of the full subsequent data set that exploits the excellent -ray spectroscopic capabilities of Gerda.

The GERmanium Detector Array ( Gerda ) experiment operated enriched high-purity germanium detectors in a liquid argon cryostat, which contains 0.33% of$$^{36}$$36 Ar, a candidate isotope for the two-neutrino double-electron capture (2$$\\nu $$ν ECEC) and therefore for the neutrinoless double-electron capture (0$$\\nu $$ν ECEC). If detected, this process would give evidence of lepton number violation and the Majorana nature of neutrinos. In the radiative 0$$\\nu $$ν ECEC of$$^{36}$$36 Ar, a monochromatic photon is emitted with an energy of 429.88 keV, which may be detected by the Gerda germanium detectors. We searched for the$$^{36}$$36 Ar 0$$\\nu $$ν ECEC with Gerda data, with a total live time of 4.34 year (3.08 year accumulated during Gerda Phase II and 1.26 year during Gerda Phase I). No signal was found and a 90% CL lower limit on the half-life of this process was established$$T_{1/2} >1.5\\cdot 10^{22} $$T 1 / 2 > 1.5 · 10 22  year.

The beta decay of $$^{77}$$ 77Ge and $$^{77\\textrm{m}}$$ 77mGe, both produced by neutron capture on $$^{76}$$ 76Ge, is a potential background for Germanium based neutrinoless double-beta decay search experiments such as GERDA or the LEGEND experiment. In this work we present a search for $$^{77}$$ 77Ge decays in the full GERDA Phase II data set. A delayed coincidence method was employed to identify the decay of $$^{77}$$ 77Ge via the isomeric state of $$^{77}$$ 77As ( $$9/2^+$$ 9/2+, $${475}\\,\\hbox {keV}$$ 475keV, $${T_{1/2} = {114}\\,{\\upmu }\\hbox {s}}$$ T1/2=114μs, $$^{77\\textrm{m}}$$ 77mAs). New digital signal processing methods were employed to select and analyze pile-up signals. No signal was observed, and an upper limit on the production rate of $$^{77}$$ 77Ge was set at $$<0.216$$ <0.216 nuc/(kg $$\\cdot $$ · yr) (90% CL). This corresponds to a total production rate of $$^{77}$$ 77Ge and $$^{77\\textrm{m}}$$ 77mGe of $$<{0.38}$$ <0.38 nuc/(kg $$\\cdot $$ · yr) (90% CL), assuming equal production rates. A previous Monte Carlo study predicted a value for in-situ $$^{77}$$ 77Ge and $$^{77\\textrm{m}}$$ 77mGe production of (0.21 ± 0.07) nuc/(kg.yr), a prediction that is now further corroborated by our experimental limit. Moreover, tagging the isomeric state of $$^{77\\textrm{m}}$$ 77mAs can be utilised to further suppress the $$^{77}$$ 77Ge background. Considering the similar experimental configurations of LEGEND-1000 and GERDA, the cosmogenic background in LEGEND-1000 at LNGS is estimated to remain at a sub-dominant level.