1998
DOI: 10.1016/s0920-5632(98)00034-6
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Search for ββ in 136Xe: new data, analysis and results from the Gotthard experiment

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Cited by 8 publications
(2 citation statements)
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“…Other materials or locations in the detector array are negligible due their small masses and low activities. The following background components were simulated: the natural decay chains of 238 U and 232 Th, 40 K, cosmogenic and anthropogenic isotopes, muon showers and neutron induced interactions. It was assumed that the 238 U and 232 Th decay chains are in secular equilibrium and that the radioactive isotopes in the respective materials are uniformly distributed.…”
Section: Background Modelmentioning
confidence: 99%
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“…Other materials or locations in the detector array are negligible due their small masses and low activities. The following background components were simulated: the natural decay chains of 238 U and 232 Th, 40 K, cosmogenic and anthropogenic isotopes, muon showers and neutron induced interactions. It was assumed that the 238 U and 232 Th decay chains are in secular equilibrium and that the radioactive isotopes in the respective materials are uniformly distributed.…”
Section: Background Modelmentioning
confidence: 99%
“…The measured neutron flux in the Gran Sasso underground laboratory [19] was simulated using the MICAP implementation in Geant [20]. The activities of 40 K and 210 Pb in the LC2-Pb shield were determined in separate activity measurements [21]. In order to extract the best fit values for each activity, a least-squares method has been used.…”
Section: Background Modelmentioning
confidence: 99%