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4 result(s) for "Oldorf, C"
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Current Status and Future Perspectives of the COBRA Experiment
The aim of the COBRA experiment is to prove the existence of neutrinoless double-beta-decay (0νββ-decay) and to measure its half-life. For this purpose a detector array made of cadmium-zinc-telluride (CdZnTe) semiconductor detectors is operated at the Gran Sasso Underground Laboratory (LNGS) in Italy. This setup is used to investigate the experimental issues of operating CdZnTe detectors in low-background mode and to identify potential background components, whilst additional studies are proceeding in surface laboratories. The experiment currently consists of monolithic, calorimetric detectors of coplanar grid design (CPG detectors). These detectors are 1 × 1 × 1 cm3 and are arranged in 4 × 4 detector layers. Ultimately four layers will be installed by the end of 2013, of which two are currently operating. To date 82.3 kg·days of data have been collected. In the region of interest for 116Cd around 2.8 MeV, the median energy resolution is 1.5% FWHM, and a background level near 1 counts/keV/kg/y has been reached. This paper gives an overview of the current status of the experiment and future perspectives.
Characterization of a large CdZnTe coplanar quad-grid semiconductor detector
The COBRA collaboration aims to search for neutrinoless double beta-decay of \\(^{116}\\)Cd. A demonstrator setup with 64 CdZnTe semiconductor detectors, each with a volume of 1cm\\(^3\\), is currently being operated at the LNGS underground laboratory in Italy. This paper reports on the characterization of a large (2 \\(\\times\\) 2 \\(\\times\\) 1.5)cm\\(^3\\) CdZnTe detector with a new coplanar-grid design for applications in \\(\\gamma\\)-ray spectroscopy and low-background operation. Several studies of electric properties as well as of the spectrometric performance, like energy response and resolution, are conducted. Furthermore, measurements including investigating the operational stability and a possibility to identify multiple-scattered photons are presented.
The COBRA demonstrator at the LNGS underground laboratory
The COBRA demonstrator, a prototype for a large-scale experiment searching for neutrinoless double beta-decay, was built at the underground laboratory Laboratori Nazionali del Gran Sasso (LNGS) in Italy. It consists of an array of 64 monolithic, calorimetric CdZnTe semiconductor detectors with a coplanar-grid design and a total mass of 380g. It is used to investigate the experimental challenges faced when operating CdZnTe detectors in low-background mode, to identify potential background sources and to show the long-term stability of the detectors. The first data-taking period started in 2011 with a subset of the detectors, while the demonstrator was completed in November 2013. To date, more than 250kg d of data have been collected. This paper describes technical details of the experimental setup and the hardware components.
Long-Term Stability of Underground Operated CZT Detectors Based on the Analysis of Intrinsic \\(^{113}\\)Cd \\beta\\(^{-}\\)-Decay
The COBRA collaboration operates a demonstrator setup at the underground facility LNGS (Laboratori Nazionali del Gran Sasso, located in Italy) to prove the technological capabilities of this concept for the search for neutrinoless double beta-decay. The setup consists of 64 \\((1\\times\\!1\\times\\!1)\\) cm\\(^{3}\\) CZT detectors in CPG configuration. One purpose of this demonstrator is to test if reliable long-term operation of CZT-CPG detectors in such a setup is possible. The demonstrator has been operated under ultra low-background conditions since more than three years and collected data corresponding to an exposure of 218 kg\\(\\cdot\\)days. The presented study focuses on the long-term stability of CZT detectors by analyzing the intrinsic, fourfold forbidden non-unique \\(^{113}\\)Cd single beta-decay. It can be shown that CZT detectors can be operated stably for long periods of time and that the \\(^{113}\\)Cd single beta-decay can be used as an internal monitor of the detector performance during the runtime of the experiment.