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72 5 Scintilla<strong>to</strong>r <strong>upgrade</strong><br />

In 3.1 % of the simulated double beta decay events, two CZT and no CsI<br />

crystals were involved. 1 % of all double beta events deposit energy in<br />

a 3σ interval aro<strong>und</strong> 1294 keV in one CZT crystal and an energy of less<br />

than 1511 keV in another CZT crystal.<br />

76.77 % of all 116 Cd decays in<strong>to</strong> the first excited state produce coincident<br />

hits in the CZT and scintillation detec<strong>to</strong>rs. 47.60 % and 17.00 % of<br />

all events deposit energy in one CZT and one or two CsI crystals. Further<br />

studies will consider coincident hits with one CZT and one or two<br />

CsI detec<strong>to</strong>r hits, being 64.6 % of the <strong>to</strong>tal amount of events. Coincident<br />

hits are defined in the simulation as hits in the CZT and CsI detec<strong>to</strong>rs,<br />

that belong <strong>to</strong> one event, whereas in the experiment these will be hits<br />

(belonging <strong>to</strong> a single decay or not) in multiple detec<strong>to</strong>rs within a time<br />

window of several tens of µs. For low count rates and small time windows,<br />

random coincidences are strongly suppressed.<br />

Events with deposited energy of up <strong>to</strong> the electron endpoint energy<br />

of 1511 keV in one CZT detec<strong>to</strong>r and an energy deposition of aro<strong>und</strong><br />

1294 keV in the CsI detec<strong>to</strong>rs are the majority of all coincident events.<br />

By considering an interval of 3σ (5σ) aro<strong>und</strong> the 1294 keV gamma line<br />

in the CsI detec<strong>to</strong>rs 43.4 % (50.8 %) of all coincident (1CZT and 1&2CsI)<br />

events and 28.0 % (32.9 %) of all signal events are included.<br />

In figure 5.9 the deposited energy of the CZT is plotted against the energy<br />

entry of the scintillation detec<strong>to</strong>rs, if only one CZT and one or two<br />

CsI crystals were involved.<br />

The red lines mark a distance of 3σ <strong>to</strong> the expected full energy deposition<br />

of the 1294 keV pho<strong>to</strong>n in the CsI crystal. The standard derivation<br />

from equation (5.2) at 1294 keV was used. The interval between the red<br />

limes contains 99.7 % of all energy depositions with an expected value<br />

of 1294 keV.<br />

Cut ECZT (keV) ECsI(keV ) ECZT + ECsI (keV) ɛ (%)<br />

A-3σ - 1231-1357 - 28.0<br />

A-5σ - 1190-1398 - 32.9<br />

B-3σ - 1231-1357 >2200 2.9<br />

B-5σ - 1190-1398 >2200 3.4<br />

C-3σ 300-900 1231-1357 - 26.2<br />

C-5σ 300-900 1190-1398 - 27.6<br />

Table 5.6: Efficiencies <strong>for</strong> different cuts <strong>for</strong> events in one CZT and one<br />

or two CsI detec<strong>to</strong>r.

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