Germanium Detector Array: Difference between revisions

Content deleted Content added
Lxplot (talk | contribs)
mNo edit summary
details
Line 1:
{{Underlinked|date=December 2014}}
 
The GERmanium Detector Array ('''GERDA''') experiment is searching for [[neutrinoless double beta decay]](0vββ) in Ge-76 at the underground [[Laboratori Nazionali del Gran Sasso]] (LNGS). [[Neutrinoless beta decay]] is expected to be a very rare process if possibleit occurs. The collocationcollaboration predicts less than one event each year per kilogram of material, appearing as a narrow spike around 2039 keV in the observed energy spectrum. This means b[[Radiation_protection|Backgroundackground shielding]] is required to detect any rare decays. The LNGS facility has 1400 meters of rock overburden, equivalent to 3000 meters of water shielding, reducing [[Cosmic ray|cosmic radiation]] [[Background radiation|background]].
 
== Design ==
The experiment uses high purity enriched [[Germanium|Ge]] crystal [[diodes]] (HPGe) as a beta decay source and [[particle detector]]. The detectors from the HdM and Igex experiments were reprocessed and used in GERDAphase 1. The detector array is suspended in a liquid [[argon]] [[cryostat]] lined with copper and surrounded by an ultra-pure water tank. [[Photomultiplier|PMTs]] in the water tank and plastic [[scintillators]] above detect and exclude background [[muons]].
 
Phase 2 will increase the active mass to 38kg using 30 new HPGe detectors. A magnitude reduction in background is planned to 10<sup>-3</sup>/(keV·kg·yr) using cleaner materials. This will increase the half-life sensitivity to 10<sup>26</sup> years once 100kg·yr of data is taken and enable evaluation of possible ton-scale expansion.
 
== Results ==
 
Phase I collected data November 2011 to May 2013, with 21.6&nbsp;kg·yr exposure, obtaining a 0vββ 90% CL half-life limit of:
 
<math>T_{0 \nu \beta \beta} > 2.1*10^{2125} yr </math>. This limit can be combined with previous results, disfavouringdisfavoring the Heidelberg-Moscow experiment detection claim. A double beta decay half-life was also measured: T<sub>2vββ</sub> = (1.84<sup>+0.14</sup><sub>−0.10</sub>)·10<sup>21</sup> yr.
 
Phase II will have additional enriched Ge detectors and reduced background, raising the sensitivity about one order.
 
== Publications ==