COBRA Experiment
{{Infobox Laboratory
| name = Cadmium Zinc Telluride 0-Neutrino Double-Beta Research Apparatus
| motto =
| image =
| established =
| director =
| city = L'Aquila
| province = Abruzzo
| country = Italy
| coor = {{coord|42.454|13.576|region:IT-65_type:mountain_source:ETRF2000(X4582167.465,Y1106521.805,Z4283602.714)|display=it}}
| budget =
| type = Particle physics, Astrophysics
| staff =
| campus =
| operating_agency = INFN
| website = {{URL|http://www.cobra-experiment.org/}}
}}
The Cadmium Zinc Telluride 0-Neutrino Double-Beta (COBRA) experiment is a large array of cadmium zinc telluride (CdZnTe) semiconductors searching for evidence of neutrinoless double beta decay and to measure its half-life. COBRA is located underground, within the Gran Sasso National Laboratory. The experiment was proposed in 2001, and installation of a large prototype began in 2006.{{Cite journal|last=Wilson|first=J. R.|date=2008|title=The COBRA experiment|url=http://stacks.iop.org/1742-6596/120/i=5/a=052048|journal=Journal of Physics: Conference Series|language=en|volume=120|issue=5|pages=052048|doi=10.1088/1742-6596/120/5/052048|issn=1742-6596|doi-access=free}}
Set up
COBRA is designed to prove the validity of the CdZnTe detection technique.{{Cite journal|last1=Ebert|first1=J.|last2=Fritts|first2=M.|display-authors=1|date=2016-01-21|title=The COBRA demonstrator at the LNGS underground laboratory|journal=Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment|volume=807|pages=114–120|doi=10.1016/j.nima.2015.10.079|issn=0168-9002|bibcode=2016NIMPA.807..114E|arxiv=1507.08177|s2cid=110688200}} The initial setup of the experiment, in 2007, was an array of four 1-cm3 CdZnTe semiconductors.{{Cite journal|last1=Bloxham|first1=T.|last2=Boston|first2=A.|display-authors=1|date=2007-08-03|title=First results on double β-decay modes of Cd, Te, and Zn Isotopes|journal=Physical Review C|volume=76|issue=2|pages=025501|doi=10.1103/PhysRevC.76.025501|arxiv=0707.2756|bibcode=2007PhRvC..76b5501B|s2cid=119257817}} This was then upgraded to 64 detectors in a 4×4×4 array. The CdZnTe crystals act as both the detector and source material, as nine of the isotopes in this material are double beta decay candidates.{{Cite journal|last1=Ebert|first1=J.|last2=Fritts|first2=M.|last3=Gößling|first3=C.|last4=Göpfert|first4=T.|last5=Gehre|first5=D.|last6=Hagner|first6=C.|last7=Heidrich|first7=N.|last8=Köttig|first8=T.|last9=Neddermann|first9=T.|display-authors=1|date=2013|title=Current Status and Future Perspectives of the COBRA Experiment|journal=Advances in High Energy Physics|language=en|volume=2013|pages=1–6|doi=10.1155/2013/703572|issn=1687-7357|doi-access=free}} The location of the experiment allows for shielding from external gamma rays; to this end, the detectors are also shielded by 5 cm of radiopure electrolytic copper and 20 cm of low-radioactivity lead. 7 cm of boron-loaded polyethylene shields the experiment against neutrons, and the experiment is constantly flushed with nitrogen gas to prevent contamination with radon.
Results
References
{{Reflist}}
External links
- [http://www.cobra-experiment.org/ Cobra Experiment home page]
{{neutrino detectors}}