Testing the Ge detectors for the MAJORANA DEMONSTRATOR
- Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
- Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)
- Pacific Northwest National Lab. (PNNL), Richland, WA (United States)
- Univ. of South Carolina, Columbia, SC (United States); Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
- Institute for Theoretical and Experimental Physics, Moscow (Russia)
- Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
- Joint Institute for Nuclear Research, Dubna (Russia)
- Duke Univ., Durham, NC (United States); Triangle Univ. Nuclear Lab., Durham, NC (United States)
- Univ. of South Dakota, Vermillion, SD (United States)
- South Dakota School of Mines and Technology, Rapid City, SD (United States)
- North Carolina State Univ., Raleigh, NC (United States); Triangle Univ. Nuclear Lab., Durham, NC (United States)
- Univ. of Washington, Seattle, WA (United States)
- Univ. of Tennessee, Knoxville, TN (United States)
- Osaka Univ., Osaka (Japan)
- Univ. of North Carolina, Chapel Hill, NC (United States); Triangle Univ. Nuclear Lab., Durham, NC (United States)
- Univ. of South Carolina, Columbia, SC (United States)
- Univ. of Alberta, Edmonton, AB (Canada)
- Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States); North Carolina State Univ., Raleigh, NC (United States)
- Black Hills State Univ., Spearfish, SD (United States)
- Tennessee Tech Univ., Cookeville, TN (United States)
- Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States); Univ. of Tennessee, Knoxville, TN (United States)
- South Dakota School of Mines and Technology, Rapid City, SD (United States); Black Hills State Univ., Spearfish, SD (United States)
- Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States); Univ. of California, Berkeley, CA (United States)
- Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States); Triangle Univ. Nuclear Lab., Durham, NC (United States); Univ. of North Carolina, Chapel Hill, NC (United States)
High purity germanium (HPGe) crystals will be used for the Majorana Demonstrator, where they serve as both the source and the detector for neutrinoless double beta decay. It is crucial for the experiment to understand the performances of the HPGe crystals. A variety of crystal properties are being investigated, including both basic properties such as energy resolution, efficiency, uniformity, capacitance, leakage current and crystal axis orientation, as well as more sophisticated properties, e.g. pulse shapes and dead layer and transition layer distribution. In this talk, we will present our measurements that characterize the HPGe crystals. In addition, we will discuss the experiment’s simulation package for the detector characterization setup, where additional information is learned from data simulation comparisons.
- Research Organization:
- Los Alamos National Laboratory (LANL), Los Alamos, NM (United States); Pacific Northwest National Laboratory (PNNL), Richland, WA (United States)
- Sponsoring Organization:
- USDOE Office of Science (SC), Nuclear Physics (NP)
- Grant/Contract Number:
- AC05-76RL01830
- OSTI ID:
- 1201774
- Alternate ID(s):
- OSTI ID: 1224508
- Report Number(s):
- PNNL-SA-102131; PII: S1875389214007172
- Journal Information:
- Physics Procedia, Vol. 61, Issue C; ISSN 1875-3892
- Publisher:
- ElsevierCopyright Statement
- Country of Publication:
- United States
- Language:
- English
Web of Science
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