02.12.2012 Views

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 ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

18 3 The COBRA experiment<br />

They are commercially supplied with a red passivation, which<br />

prevents the degradation of the crystal material due <strong>to</strong> oxidation<br />

processes or moisture. This passivation has been identified as the<br />

main backgro<strong>und</strong> source in a <strong>for</strong>mer test set-up with 16 crystals.<br />

Crystals with a low backgro<strong>und</strong> optimised colourless passivation<br />

had a reduced backgro<strong>und</strong> level of about a fac<strong>to</strong>r 10 [24] and are<br />

investigated in the current set-up with eight crystals of two different<br />

passivations. The left side of figure 3.2 shows one of 64<br />

CZT detec<strong>to</strong>rs with colourless passivation, which will be installed<br />

soon.<br />

CZT detec<strong>to</strong>rs operate with a high voltage of about one kV/cm,<br />

being applied between the cathode (bot<strong>to</strong>m side of crystal in figure<br />

3.2) and a coplanar grid anode (upper side of crystal in figure<br />

3.2). CZT detec<strong>to</strong>rs with a common anode have, due <strong>to</strong> different<br />

charge carrier mobilities and trapping times, a signal, which<br />

depends on the collection time and point of interaction. Thus,<br />

a suitable energy resolution could not be obtained. The coplanar<br />

grid anode has been developed as electron-only readout (see<br />

[25]) and therewith energy resolutions of <strong>und</strong>er 1 % (FWHM at<br />

662 keV) can be achieved. Typical crystals used <strong>for</strong> the COBRA<br />

pro<strong>to</strong>type set-up have resolutions of aro<strong>und</strong> 3-5 % [8].<br />

3.3 Motivation <strong>for</strong> scintilla<strong>to</strong>r <strong>upgrade</strong><br />

Besides the 0νββ decays, the 2νββ transitions are of physical interest as<br />

well. The 2νββ decay of 116 Cd in<strong>to</strong> the first excited state is of interest<br />

<strong>for</strong> this thesis. Figure 3.3 shows the transitions of 116 Cd in<strong>to</strong> the gro<strong>und</strong><br />

and first excited state of 116 Sn. The decay of 116 Cd in<strong>to</strong> the first excited<br />

state is accompanied by the emission of a 1294 keV pho<strong>to</strong>n.<br />

The current Cobra experiment has a low efficiency <strong>for</strong> gamma ray detection.<br />

Only about every tenth of the in this decay emitted 1294 keV<br />

pho<strong>to</strong>ns interacts with the small CZT detec<strong>to</strong>rs and the full energy of<br />

these pho<strong>to</strong>ns is detected <strong>for</strong> only 1% of the decays. This leads <strong>to</strong> a<br />

small detection efficiency <strong>for</strong> this double beta decay. Accordingly, an<br />

<strong>upgrade</strong> of the current COBRA setup <strong>to</strong> enable a better gamma ray detection<br />

is desirable.<br />

The aim of this thesis is there<strong>for</strong>e <strong>to</strong> develop a <strong>design</strong> of a COBRA <strong>upgrade</strong><br />

with a high detection efficiency <strong>for</strong> the decay of 116 Cd in<strong>to</strong> the<br />

first excited state. A desired <strong>upgrade</strong> should achieve high detection ef-

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!