a design study for a cobra upgrade to - Institut für Kern- und ...
a design study for a cobra upgrade to - Institut für Kern- und ...
a design study for a cobra upgrade to - Institut für Kern- und ...
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80 5 Scintilla<strong>to</strong>r <strong>upgrade</strong><br />
and gamma ray which have each a much lower energy than the signature.<br />
The direct transition of 137 Cs <strong>to</strong> the gro<strong>und</strong> state of 137 Ba can have<br />
only a signature similar <strong>to</strong> the double beta decay event with very low<br />
electron energy.<br />
Simulations of a backgro<strong>und</strong> level of 7.5 mBq 137 Cs, corresponding <strong>to</strong><br />
7.5 × 10 6 137 Cs decays per year in the planned scintilla<strong>to</strong>rs, producing<br />
14.5×10 6 noncoincident events per year. This number of events was<br />
simulated and all events deposit energy in one or more CsI crystals.<br />
The majority of these events deposit energy in one (28.5 %), two (10.8 %)<br />
or three (1.6 %) scintilla<strong>to</strong>rs. Only 1.23 % of all 137 Cs events have also<br />
coincident entries in the CZT detec<strong>to</strong>rs. 0.39 % have entries in one CZT<br />
and one CsI and 0.53 % in one CZT and two CsI.<br />
The coincident deposited energy in CZT and CsI detec<strong>to</strong>rs can in figure<br />
5.14. The energy deposition in the CsI detec<strong>to</strong>rs is except <strong>for</strong> small<br />
energy depositions in the CZT detec<strong>to</strong>rs, below the 3σ interval aro<strong>und</strong><br />
1294 keV. The maximum deposited energy in the CZT detec<strong>to</strong>rs aro<strong>und</strong><br />
662 keV, corresponding <strong>to</strong> the full energy deposition of the 662 keV<br />
gamma ray. The pure 137 Cs backgro<strong>und</strong> contribution can already be<br />
excluded with the general CZT energy threshold of a few h<strong>und</strong>red keV.<br />
The 137 Cs contamination is there<strong>for</strong>e of minor importance, as long as<br />
the backgro<strong>und</strong> level of the hole experiment is small enough <strong>to</strong> avoid a<br />
pile up with other backgro<strong>und</strong> sources.<br />
87 RB is a primordial nucleus, decaying with a half life of 4.75 ·10 10 years<br />
through beta decay with a Q-value of 282 keV. Natural Rb includes<br />
27.8 % 87 Rb and Kim et al. [56] located contamination of 1 <strong>to</strong> 1000 ppb in<br />
different CsI powders. A reduction <strong>to</strong> 1 ppb was possible with recrystallisation<br />
of the powder with pure water. Without further reduction a<br />
contamination level of 11.8 ppb (corresponding <strong>to</strong> 12.14 mBq/kg) was<br />
reported. Accordingly 12 × 10 6 decays per year are expected in the<br />
extended COBRA detec<strong>to</strong>r. The single decays of 87 Rb are no serious<br />
backgro<strong>und</strong>, but might contribute as backgro<strong>und</strong> by pile up with other<br />
backgro<strong>und</strong> sources.<br />
RESULTS<br />
These estimations show, that CsI crystal, which have not been s<strong>to</strong>red<br />
<strong>und</strong>ergro<strong>und</strong> <strong>for</strong> a few decades, cannot be easily used <strong>for</strong> searches of<br />
the neutrino accompanied double beta decay of 116 Cd in<strong>to</strong> the first excited<br />
state of 116 Sn. These estimations were made <strong>for</strong> already backgro<strong>und</strong><br />
reduced crystals. For crystals that are not backgro<strong>und</strong> reduced,