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a design study for a cobra upgrade to - Institut für Kern- und ...

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5.3 Monte Carlo studies of the <strong>design</strong>ed <strong>upgrade</strong> 83<br />

decay chains produce 0.03 % and 0.04 % coincident (1CZT-1&2CsI) entries,<br />

being about 15000 and 7000 coincident events.<br />

Accordingly, the PMTs could become a main source of backgro<strong>und</strong> and<br />

their use should be avoided.<br />

PAINT: The upper limit <strong>for</strong> contamination in the colourless paint <strong>for</strong><br />

the CZT crystal was measured <strong>to</strong> be lower than 1.5 mBq/kg <strong>for</strong> 238 U,<br />

0.6 mBq/kg <strong>for</strong> 232 Th and 50 mBq/kg <strong>for</strong> 40 K [58], resulting in less<br />

than about 220000, 11000 and 55000 decays per year (paint mass of<br />

0.027g/CZT crystal). Less than 5 % of these decays produce coincident<br />

entries, whereas about 100 are in the cut C-3σ region.<br />

222 RN decays with a half-life of 3.82 days, but feeds in<strong>to</strong> 210 Pb with a<br />

half-life of 22 years. The last gamma active nuclei in the 222 Rn decay<br />

chain is 214 Bi. As Rn is a gas, it diffuses in<strong>to</strong> every area with lower partial<br />

pressure. The decay product will be charged and accumulate on all<br />

surfaces. The air in the Gran Sasso labora<strong>to</strong>ry can have radon activities<br />

of 35±2 Bq/m 3 [20]. The cavity in the Nest contains roughly 4·10 −4 m 3 ,<br />

yielding about 15 mBq or half a million 222 Rn decays in one year. These<br />

is a maximal estimation, without nitrogen flushing. Simulation of one<br />

million events of the 222 Rn decay chain in the Nest air were produced.<br />

3 % of these decays produce coincident (1CZT-1&2CsI) entries. These<br />

decays will produce about 520 events in the C-3σ region, being less than<br />

7 % of the minimal expected 134 Cs backgro<strong>und</strong>.<br />

RESULTS<br />

Backgro<strong>und</strong> PMT (K/U/Th) Paint (K/U/Th) 222 Rn<br />

activity 504/78.2/25.5 mBq/PMT 4/0.1/1 Bq/kg 35 mBq/m 3<br />

events/year 318/50/17×10 6 0.2/0.1/0.06×10 6 0.5×10 6<br />

1CZT-1&2CsI 0.04/0.03/0.04 % ?/3.2/4.6 % 2.95 %<br />

Table 5.11: List of different backgro<strong>und</strong> sources<br />

The detection of the neutrinoless double beta decay in<strong>to</strong> the first excited<br />

state is not possible or at least very difficult with CsI crystals. The<br />

backgro<strong>und</strong> of 134 Cs is more than one order of magnitude higher than<br />

the upper limits of the paint and 222 Rn backgro<strong>und</strong>.<br />

As alternative scintilla<strong>to</strong>r CWO or BGO should be studied. NaI:Tl is<br />

due <strong>to</strong> is small density and the preferred read out with PMTs no solution,<br />

as even backgro<strong>und</strong> optimised PMTs are expected <strong>to</strong> be a main

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