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001     408376
005     20211110151247.0
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020 _ _ |a 978-3-935702-83-6
024 7 _ |a 10.3204/DESY-PROC-2013-04/walter_manuel
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024 7 _ |a 1435-8077
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041 _ _ |a English
088 1 _ |a DESY-PROC-2013-04
088 _ _ |a DESY-PROC-2013-04
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100 1 _ |a Walter, Michael
|b 0
111 2 _ |a 9th Patras Workshop on Axions, WIMPs and WISPs
|c Mainz
|d 2013-06-24 - 2013-06-28
|g AXION-WIMP 2013
|0 C13-06-24.5
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245 _ _ |a The Gerda Experiment for the Search of Neutrinoless Double Beta Decay
260 _ _ |a Hamburg
|c 2013
|b Verlag Deutsches Elektronen-Synchrotron
295 1 0 |a Walter, M. "The Gerda Experiment for the Search of Neutrinoless Double Beta Decay" in Proceedings, 9th Patras Workshop on Axions, WIMPs and WISPs (AXION-WIMP 2013) / Oberlack, Uwe, Sissol, Pierre (eds.), 2013 ; AXION-WIMP 2013 : 9th Patras Workshop on Axions, WIMPs and WISPs , 2013-06-23 - 2013-06-28, Mainz
300 _ _ |a 281-286
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520 _ _ |a The Gerda experiment, situated at Laboratori Nazionali del Gran Sasso is designed to search for the neutrinoless double $\beta$ decay. Bare high purity Ge-diodes enriched to 86 %in $^{76}Ge$ are directly immersed into liquid Ar. Phase I operated from November 2011 till May 2013 yielding an exposure of 21.6 kg·yr, with a mean background near the Q-value of2·$10^{−2}$ cts/(keV·kg·yr). A half-life of $1.84^{−0.10}_{+0.14}·10^{21}$ yr was recently published for the two-neutrino double $\beta$ decay. For Phase II, additional 20 kg of broad-energy Ge detectors will be installed to reach an exposure of 100 kg·yr with one order of magnitude less background, exploring half-lifes up to 1.5·$10^{26}$ yr. This will be achieved by liquid Ar instrumentation as an active veto, pulse shape analysis and a refined selection of radio-pure materials.
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700 1 _ |a Gerda Collaboration
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787 0 _ |a Oberlack, Uwe et. al.
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|t Proceedings, 9th Patras Workshop on Axions, WIMPs and WISPs (AXION-WIMP 2013)
856 4 _ |u https://bib-pubdb1.desy.de/record/408376/files/fulltext.pdf
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