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12 3 The COBRA experiment<br />

CdZnTe (CZT) contains nine double beta decay iso<strong>to</strong>pes, which are<br />

listed in table 3.1 with their natural ab<strong>und</strong>ance, the possible decay<br />

mode and the Q-value.<br />

Iso<strong>to</strong>pe Q (keV) nat. ab. (%) decay mode<br />

64 Zn 1096 48.6 EC/EC, EC/β +<br />

70 Zn 1001 0.6 β − β −<br />

106 Cd 2771 1.3 EC/EC, EC/β + , β + β +<br />

108 Cd 231 0.9 EC/EC<br />

114 Cd 534 28.7 β − β −<br />

116 Cd 2805 7.5 β − β −<br />

120 Te 1722 0.1 EC/EC, EC/β +<br />

128 Te 868 31.7 β − β −<br />

130 Te 2529 33.8 β − β −<br />

Table 3.1: Double beta iso<strong>to</strong>pes of relevance <strong>for</strong> the COBRA experiment,<br />

with Q-value, natural ab<strong>und</strong>ance and possible decay mode given<br />

according <strong>to</strong> Kiel [8].<br />

The most promising iso<strong>to</strong>pes <strong>for</strong> the COBRA experiment are 116 Cd and<br />

130 Te. Their decays have a high Q-value, which is favourable <strong>for</strong> the<br />

expected event rate as it varies with Q 5 <strong>for</strong> 0νββ. Additionally, 116 Cd<br />

has, with 2805 keV, an endpoint energy well over the highest occurring<br />

natural gamma line at 2614 keV from the 232 Th decay chain [16]. The<br />

Q-value of 130 Te is between this line and its Comp<strong>to</strong>n edge. This leads<br />

<strong>to</strong> a reduced backgro<strong>und</strong> <strong>for</strong> their expected 0νβ − β − gro<strong>und</strong> state transitions.<br />

A natural high ab<strong>und</strong>ance of 130 Te provides also relatively high<br />

source mass, already without using iso<strong>to</strong>pically enriched material. CZT<br />

contains also 106 Cd, which is one of only 6 known β + β + decay iso<strong>to</strong>pes.<br />

CdZnTe crystals are intrinsic II-VI semiconduc<strong>to</strong>r crystals with a zinc<br />

blende structure. They are produced by the High Pressure Bridgman<br />

Method with low intrinsic contamination, but also with a limited detec<strong>to</strong>r<br />

size of a few cm 3 . This requires a modular <strong>design</strong> <strong>for</strong> reaching<br />

high source mass, <strong>for</strong> which the collaboration investigates the advantages<br />

of a coincidence analysis. Owing <strong>to</strong> a large band gap of 1.6 eV,<br />

CZT detec<strong>to</strong>rs can be operated at room temperature, which avoids extensive<br />

cooling.<br />

Currently, different CZT detec<strong>to</strong>r <strong>design</strong>s are <strong>und</strong>er investigation.<br />

These are coplanar grid CZT detec<strong>to</strong>rs, which will be discussed further<br />

on and two different pixelated <strong>design</strong>s, which show promising possibilities<br />

of a very effective backgro<strong>und</strong> reduction. For the recent activities

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