Low radioactive material screening and background control for the PandaX-4T experiment
Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, IC...
Ausführliche Beschreibung
Autor*in: |
Qian, Zhicheng [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2022 |
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Schlagwörter: |
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Anmerkung: |
© The Author(s) 2022 |
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Übergeordnetes Werk: |
Enthalten in: Journal of high energy physics - Berlin : Springer, 1997, 2022(2022), 6 vom: 27. Juni |
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Übergeordnetes Werk: |
volume:2022 ; year:2022 ; number:6 ; day:27 ; month:06 |
Links: |
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DOI / URN: |
10.1007/JHEP06(2022)147 |
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Katalog-ID: |
SPR047438754 |
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520 | |a Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. | ||
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700 | 1 | |a Si, Lin |4 aut | |
700 | 1 | |a Abdukerim, Abdusalam |4 aut | |
700 | 1 | |a Bo, Zihao |4 aut | |
700 | 1 | |a Chen, Wei |4 aut | |
700 | 1 | |a Chen, Xun |4 aut | |
700 | 1 | |a Chen, Yunhua |4 aut | |
700 | 1 | |a Cheng, Chen |4 aut | |
700 | 1 | |a Cheng, Yunshan |4 aut | |
700 | 1 | |a Cui, Xiangyi |4 aut | |
700 | 1 | |a Fan, Yingjie |4 aut | |
700 | 1 | |a Fang, Deqing |4 aut | |
700 | 1 | |a Fu, Changbo |4 aut | |
700 | 1 | |a Fu, Mengting |4 aut | |
700 | 1 | |a Geng, Lisheng |4 aut | |
700 | 1 | |a Giboni, Karl |4 aut | |
700 | 1 | |a Gu, Linhui |4 aut | |
700 | 1 | |a Guo, Xuyuan |4 aut | |
700 | 1 | |a Han, Ke |4 aut | |
700 | 1 | |a He, Changda |4 aut | |
700 | 1 | |a He, Jinrong |4 aut | |
700 | 1 | |a Huang, Di |4 aut | |
700 | 1 | |a Huang, Yanlin |4 aut | |
700 | 1 | |a Huang, Zhou |4 aut | |
700 | 1 | |a Hou, Ruquan |4 aut | |
700 | 1 | |a Ji, Xiangdong |4 aut | |
700 | 1 | |a Ju, Yonglin |4 aut | |
700 | 1 | |a Li, Chenxiang |4 aut | |
700 | 1 | |a Li, Mingchuan |4 aut | |
700 | 1 | |a Li, Shu |4 aut | |
700 | 1 | |a Li, Shuaijie |4 aut | |
700 | 1 | |a Lin, Qing |4 aut | |
700 | 1 | |a Liu, Jianglai |4 aut | |
700 | 1 | |a Lu, Xiaoying |4 aut | |
700 | 1 | |a Luo, Lingyin |4 aut | |
700 | 1 | |a Ma, Wenbo |4 aut | |
700 | 1 | |a Ma, Yugang |4 aut | |
700 | 1 | |a Mao, Yajun |4 aut | |
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700 | 1 | |a Ning, Xuyang |4 aut | |
700 | 1 | |a Qi, Ningchun |4 aut | |
700 | 1 | |a Ren, Xiangxiang |4 aut | |
700 | 1 | |a Shaheed, Nasir |4 aut | |
700 | 1 | |a Shang, Changsong |4 aut | |
700 | 1 | |a Shen, Guofang |4 aut | |
700 | 1 | |a Sun, Wenliang |4 aut | |
700 | 1 | |a Tan, Andi |4 aut | |
700 | 1 | |a Tao, Yi |4 aut | |
700 | 1 | |a Wang, Anqing |4 aut | |
700 | 1 | |a Wang, Meng |4 aut | |
700 | 1 | |a Wang, Qiuhong |4 aut | |
700 | 1 | |a Wang, Shaobo |4 aut | |
700 | 1 | |a Wang, Siguang |4 aut | |
700 | 1 | |a Wang, Wei |4 aut | |
700 | 1 | |a Wang, Xiuli |4 aut | |
700 | 1 | |a Wang, Zhou |4 aut | |
700 | 1 | |a Wu, Mengmeng |4 aut | |
700 | 1 | |a Wu, Weihao |4 aut | |
700 | 1 | |a Xia, Jingkai |4 aut | |
700 | 1 | |a Xiao, Mengjiao |4 aut | |
700 | 1 | |a Xiao, Xiang |4 aut | |
700 | 1 | |a Xie, Pengwei |4 aut | |
700 | 1 | |a Yan, Binbin |4 aut | |
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700 | 1 | |a Yang, Yong |4 aut | |
700 | 1 | |a Yu, Chunxu |4 aut | |
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700 | 1 | |a Yuan, Ying |4 aut | |
700 | 1 | |a Zhang, Dan |4 aut | |
700 | 1 | |a Zhang, Minzhen |4 aut | |
700 | 1 | |a Zhang, Peng |4 aut | |
700 | 1 | |a Zhang, Tao |4 aut | |
700 | 1 | |a Zhao, Li |4 aut | |
700 | 1 | |a Zheng, Qibin |4 aut | |
700 | 1 | |a Zhou, Jifang |4 aut | |
700 | 1 | |a Zhou, Ning |4 aut | |
700 | 1 | |a Zhou, Xiaopeng |4 aut | |
700 | 1 | |a Zhou, Yong |4 aut | |
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10.1007/JHEP06(2022)147 doi (DE-627)SPR047438754 (SPR)JHEP06(2022)147-e DE-627 ger DE-627 rakwb eng Qian, Zhicheng verfasserin aut Low radioactive material screening and background control for the PandaX-4T experiment 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2022 Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. Dark Matter and Double Beta Decay (experiments) (dpeaa)DE-He213 Rare Decay (dpeaa)DE-He213 Si, Lin aut Abdukerim, Abdusalam aut Bo, Zihao aut Chen, Wei aut Chen, Xun aut Chen, Yunhua aut Cheng, Chen aut Cheng, Yunshan aut Cui, Xiangyi aut Fan, Yingjie aut Fang, Deqing aut Fu, Changbo aut Fu, Mengting aut Geng, Lisheng aut Giboni, Karl aut Gu, Linhui aut Guo, Xuyuan aut Han, Ke aut He, Changda aut He, Jinrong aut Huang, Di aut Huang, Yanlin aut Huang, Zhou aut Hou, Ruquan aut Ji, Xiangdong aut Ju, Yonglin aut Li, Chenxiang aut Li, Mingchuan aut Li, Shu aut Li, Shuaijie aut Lin, Qing aut Liu, Jianglai aut Lu, Xiaoying aut Luo, Lingyin aut Ma, Wenbo aut Ma, Yugang aut Mao, Yajun aut Meng, Yue (orcid)0000-0001-9601-1983 aut Ning, Xuyang aut Qi, Ningchun aut Ren, Xiangxiang aut Shaheed, Nasir aut Shang, Changsong aut Shen, Guofang aut Sun, Wenliang aut Tan, Andi aut Tao, Yi aut Wang, Anqing aut Wang, Meng aut Wang, Qiuhong aut Wang, Shaobo aut Wang, Siguang aut Wang, Wei aut Wang, Xiuli aut Wang, Zhou aut Wu, Mengmeng aut Wu, Weihao aut Xia, Jingkai aut Xiao, Mengjiao aut Xiao, Xiang aut Xie, Pengwei aut Yan, Binbin aut Yan, Xiyu aut Yang, Jijun aut Yang, Yong aut Yu, Chunxu aut Yuan, Jumin aut Yuan, Ying aut Zhang, Dan aut Zhang, Minzhen aut Zhang, Peng aut Zhang, Tao aut Zhao, Li aut Zheng, Qibin aut Zhou, Jifang aut Zhou, Ning aut Zhou, Xiaopeng aut Zhou, Yong aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2022(2022), 6 vom: 27. Juni (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2022 year:2022 number:6 day:27 month:06 https://dx.doi.org/10.1007/JHEP06(2022)147 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2022 2022 6 27 06 |
spelling |
10.1007/JHEP06(2022)147 doi (DE-627)SPR047438754 (SPR)JHEP06(2022)147-e DE-627 ger DE-627 rakwb eng Qian, Zhicheng verfasserin aut Low radioactive material screening and background control for the PandaX-4T experiment 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2022 Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. Dark Matter and Double Beta Decay (experiments) (dpeaa)DE-He213 Rare Decay (dpeaa)DE-He213 Si, Lin aut Abdukerim, Abdusalam aut Bo, Zihao aut Chen, Wei aut Chen, Xun aut Chen, Yunhua aut Cheng, Chen aut Cheng, Yunshan aut Cui, Xiangyi aut Fan, Yingjie aut Fang, Deqing aut Fu, Changbo aut Fu, Mengting aut Geng, Lisheng aut Giboni, Karl aut Gu, Linhui aut Guo, Xuyuan aut Han, Ke aut He, Changda aut He, Jinrong aut Huang, Di aut Huang, Yanlin aut Huang, Zhou aut Hou, Ruquan aut Ji, Xiangdong aut Ju, Yonglin aut Li, Chenxiang aut Li, Mingchuan aut Li, Shu aut Li, Shuaijie aut Lin, Qing aut Liu, Jianglai aut Lu, Xiaoying aut Luo, Lingyin aut Ma, Wenbo aut Ma, Yugang aut Mao, Yajun aut Meng, Yue (orcid)0000-0001-9601-1983 aut Ning, Xuyang aut Qi, Ningchun aut Ren, Xiangxiang aut Shaheed, Nasir aut Shang, Changsong aut Shen, Guofang aut Sun, Wenliang aut Tan, Andi aut Tao, Yi aut Wang, Anqing aut Wang, Meng aut Wang, Qiuhong aut Wang, Shaobo aut Wang, Siguang aut Wang, Wei aut Wang, Xiuli aut Wang, Zhou aut Wu, Mengmeng aut Wu, Weihao aut Xia, Jingkai aut Xiao, Mengjiao aut Xiao, Xiang aut Xie, Pengwei aut Yan, Binbin aut Yan, Xiyu aut Yang, Jijun aut Yang, Yong aut Yu, Chunxu aut Yuan, Jumin aut Yuan, Ying aut Zhang, Dan aut Zhang, Minzhen aut Zhang, Peng aut Zhang, Tao aut Zhao, Li aut Zheng, Qibin aut Zhou, Jifang aut Zhou, Ning aut Zhou, Xiaopeng aut Zhou, Yong aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2022(2022), 6 vom: 27. Juni (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2022 year:2022 number:6 day:27 month:06 https://dx.doi.org/10.1007/JHEP06(2022)147 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2022 2022 6 27 06 |
allfields_unstemmed |
10.1007/JHEP06(2022)147 doi (DE-627)SPR047438754 (SPR)JHEP06(2022)147-e DE-627 ger DE-627 rakwb eng Qian, Zhicheng verfasserin aut Low radioactive material screening and background control for the PandaX-4T experiment 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2022 Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. Dark Matter and Double Beta Decay (experiments) (dpeaa)DE-He213 Rare Decay (dpeaa)DE-He213 Si, Lin aut Abdukerim, Abdusalam aut Bo, Zihao aut Chen, Wei aut Chen, Xun aut Chen, Yunhua aut Cheng, Chen aut Cheng, Yunshan aut Cui, Xiangyi aut Fan, Yingjie aut Fang, Deqing aut Fu, Changbo aut Fu, Mengting aut Geng, Lisheng aut Giboni, Karl aut Gu, Linhui aut Guo, Xuyuan aut Han, Ke aut He, Changda aut He, Jinrong aut Huang, Di aut Huang, Yanlin aut Huang, Zhou aut Hou, Ruquan aut Ji, Xiangdong aut Ju, Yonglin aut Li, Chenxiang aut Li, Mingchuan aut Li, Shu aut Li, Shuaijie aut Lin, Qing aut Liu, Jianglai aut Lu, Xiaoying aut Luo, Lingyin aut Ma, Wenbo aut Ma, Yugang aut Mao, Yajun aut Meng, Yue (orcid)0000-0001-9601-1983 aut Ning, Xuyang aut Qi, Ningchun aut Ren, Xiangxiang aut Shaheed, Nasir aut Shang, Changsong aut Shen, Guofang aut Sun, Wenliang aut Tan, Andi aut Tao, Yi aut Wang, Anqing aut Wang, Meng aut Wang, Qiuhong aut Wang, Shaobo aut Wang, Siguang aut Wang, Wei aut Wang, Xiuli aut Wang, Zhou aut Wu, Mengmeng aut Wu, Weihao aut Xia, Jingkai aut Xiao, Mengjiao aut Xiao, Xiang aut Xie, Pengwei aut Yan, Binbin aut Yan, Xiyu aut Yang, Jijun aut Yang, Yong aut Yu, Chunxu aut Yuan, Jumin aut Yuan, Ying aut Zhang, Dan aut Zhang, Minzhen aut Zhang, Peng aut Zhang, Tao aut Zhao, Li aut Zheng, Qibin aut Zhou, Jifang aut Zhou, Ning aut Zhou, Xiaopeng aut Zhou, Yong aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2022(2022), 6 vom: 27. Juni (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2022 year:2022 number:6 day:27 month:06 https://dx.doi.org/10.1007/JHEP06(2022)147 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2022 2022 6 27 06 |
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10.1007/JHEP06(2022)147 doi (DE-627)SPR047438754 (SPR)JHEP06(2022)147-e DE-627 ger DE-627 rakwb eng Qian, Zhicheng verfasserin aut Low radioactive material screening and background control for the PandaX-4T experiment 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2022 Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. Dark Matter and Double Beta Decay (experiments) (dpeaa)DE-He213 Rare Decay (dpeaa)DE-He213 Si, Lin aut Abdukerim, Abdusalam aut Bo, Zihao aut Chen, Wei aut Chen, Xun aut Chen, Yunhua aut Cheng, Chen aut Cheng, Yunshan aut Cui, Xiangyi aut Fan, Yingjie aut Fang, Deqing aut Fu, Changbo aut Fu, Mengting aut Geng, Lisheng aut Giboni, Karl aut Gu, Linhui aut Guo, Xuyuan aut Han, Ke aut He, Changda aut He, Jinrong aut Huang, Di aut Huang, Yanlin aut Huang, Zhou aut Hou, Ruquan aut Ji, Xiangdong aut Ju, Yonglin aut Li, Chenxiang aut Li, Mingchuan aut Li, Shu aut Li, Shuaijie aut Lin, Qing aut Liu, Jianglai aut Lu, Xiaoying aut Luo, Lingyin aut Ma, Wenbo aut Ma, Yugang aut Mao, Yajun aut Meng, Yue (orcid)0000-0001-9601-1983 aut Ning, Xuyang aut Qi, Ningchun aut Ren, Xiangxiang aut Shaheed, Nasir aut Shang, Changsong aut Shen, Guofang aut Sun, Wenliang aut Tan, Andi aut Tao, Yi aut Wang, Anqing aut Wang, Meng aut Wang, Qiuhong aut Wang, Shaobo aut Wang, Siguang aut Wang, Wei aut Wang, Xiuli aut Wang, Zhou aut Wu, Mengmeng aut Wu, Weihao aut Xia, Jingkai aut Xiao, Mengjiao aut Xiao, Xiang aut Xie, Pengwei aut Yan, Binbin aut Yan, Xiyu aut Yang, Jijun aut Yang, Yong aut Yu, Chunxu aut Yuan, Jumin aut Yuan, Ying aut Zhang, Dan aut Zhang, Minzhen aut Zhang, Peng aut Zhang, Tao aut Zhao, Li aut Zheng, Qibin aut Zhou, Jifang aut Zhou, Ning aut Zhou, Xiaopeng aut Zhou, Yong aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2022(2022), 6 vom: 27. Juni (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2022 year:2022 number:6 day:27 month:06 https://dx.doi.org/10.1007/JHEP06(2022)147 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2022 2022 6 27 06 |
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10.1007/JHEP06(2022)147 doi (DE-627)SPR047438754 (SPR)JHEP06(2022)147-e DE-627 ger DE-627 rakwb eng Qian, Zhicheng verfasserin aut Low radioactive material screening and background control for the PandaX-4T experiment 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2022 Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. Dark Matter and Double Beta Decay (experiments) (dpeaa)DE-He213 Rare Decay (dpeaa)DE-He213 Si, Lin aut Abdukerim, Abdusalam aut Bo, Zihao aut Chen, Wei aut Chen, Xun aut Chen, Yunhua aut Cheng, Chen aut Cheng, Yunshan aut Cui, Xiangyi aut Fan, Yingjie aut Fang, Deqing aut Fu, Changbo aut Fu, Mengting aut Geng, Lisheng aut Giboni, Karl aut Gu, Linhui aut Guo, Xuyuan aut Han, Ke aut He, Changda aut He, Jinrong aut Huang, Di aut Huang, Yanlin aut Huang, Zhou aut Hou, Ruquan aut Ji, Xiangdong aut Ju, Yonglin aut Li, Chenxiang aut Li, Mingchuan aut Li, Shu aut Li, Shuaijie aut Lin, Qing aut Liu, Jianglai aut Lu, Xiaoying aut Luo, Lingyin aut Ma, Wenbo aut Ma, Yugang aut Mao, Yajun aut Meng, Yue (orcid)0000-0001-9601-1983 aut Ning, Xuyang aut Qi, Ningchun aut Ren, Xiangxiang aut Shaheed, Nasir aut Shang, Changsong aut Shen, Guofang aut Sun, Wenliang aut Tan, Andi aut Tao, Yi aut Wang, Anqing aut Wang, Meng aut Wang, Qiuhong aut Wang, Shaobo aut Wang, Siguang aut Wang, Wei aut Wang, Xiuli aut Wang, Zhou aut Wu, Mengmeng aut Wu, Weihao aut Xia, Jingkai aut Xiao, Mengjiao aut Xiao, Xiang aut Xie, Pengwei aut Yan, Binbin aut Yan, Xiyu aut Yang, Jijun aut Yang, Yong aut Yu, Chunxu aut Yuan, Jumin aut Yuan, Ying aut Zhang, Dan aut Zhang, Minzhen aut Zhang, Peng aut Zhang, Tao aut Zhao, Li aut Zheng, Qibin aut Zhou, Jifang aut Zhou, Ning aut Zhou, Xiaopeng aut Zhou, Yong aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2022(2022), 6 vom: 27. Juni (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2022 year:2022 number:6 day:27 month:06 https://dx.doi.org/10.1007/JHEP06(2022)147 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2022 2022 6 27 06 |
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Qian, Zhicheng @@aut@@ Si, Lin @@aut@@ Abdukerim, Abdusalam @@aut@@ Bo, Zihao @@aut@@ Chen, Wei @@aut@@ Chen, Xun @@aut@@ Chen, Yunhua @@aut@@ Cheng, Chen @@aut@@ Cheng, Yunshan @@aut@@ Cui, Xiangyi @@aut@@ Fan, Yingjie @@aut@@ Fang, Deqing @@aut@@ Fu, Changbo @@aut@@ Fu, Mengting @@aut@@ Geng, Lisheng @@aut@@ Giboni, Karl @@aut@@ Gu, Linhui @@aut@@ Guo, Xuyuan @@aut@@ Han, Ke @@aut@@ He, Changda @@aut@@ He, Jinrong @@aut@@ Huang, Di @@aut@@ Huang, Yanlin @@aut@@ Huang, Zhou @@aut@@ Hou, Ruquan @@aut@@ Ji, Xiangdong @@aut@@ Ju, Yonglin @@aut@@ Li, Chenxiang @@aut@@ Li, Mingchuan @@aut@@ Li, Shu @@aut@@ Li, Shuaijie @@aut@@ Lin, Qing @@aut@@ Liu, Jianglai @@aut@@ Lu, Xiaoying @@aut@@ Luo, Lingyin @@aut@@ Ma, Wenbo @@aut@@ Ma, Yugang @@aut@@ Mao, Yajun @@aut@@ Meng, Yue @@aut@@ Ning, Xuyang @@aut@@ Qi, Ningchun @@aut@@ Ren, Xiangxiang @@aut@@ Shaheed, Nasir @@aut@@ Shang, Changsong @@aut@@ Shen, Guofang @@aut@@ Sun, Wenliang @@aut@@ Tan, Andi @@aut@@ Tao, Yi @@aut@@ Wang, Anqing @@aut@@ Wang, Meng @@aut@@ Wang, Qiuhong @@aut@@ Wang, Shaobo @@aut@@ Wang, Siguang @@aut@@ Wang, Wei @@aut@@ Wang, Xiuli @@aut@@ Wang, Zhou @@aut@@ Wu, Mengmeng @@aut@@ Wu, Weihao @@aut@@ Xia, Jingkai @@aut@@ Xiao, Mengjiao @@aut@@ Xiao, Xiang @@aut@@ Xie, Pengwei @@aut@@ Yan, Binbin @@aut@@ Yan, Xiyu @@aut@@ Yang, Jijun @@aut@@ Yang, Yong @@aut@@ Yu, Chunxu @@aut@@ Yuan, Jumin @@aut@@ Yuan, Ying @@aut@@ Zhang, Dan @@aut@@ Zhang, Minzhen @@aut@@ Zhang, Peng @@aut@@ Zhang, Tao @@aut@@ Zhao, Li @@aut@@ Zheng, Qibin @@aut@@ Zhou, Jifang @@aut@@ Zhou, Ning @@aut@@ Zhou, Xiaopeng @@aut@@ Zhou, Yong @@aut@@ |
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Qian, Zhicheng Si, Lin Abdukerim, Abdusalam Bo, Zihao Chen, Wei Chen, Xun Chen, Yunhua Cheng, Chen Cheng, Yunshan Cui, Xiangyi Fan, Yingjie Fang, Deqing Fu, Changbo Fu, Mengting Geng, Lisheng Giboni, Karl Gu, Linhui Guo, Xuyuan Han, Ke He, Changda He, Jinrong Huang, Di Huang, Yanlin Huang, Zhou Hou, Ruquan Ji, Xiangdong Ju, Yonglin Li, Chenxiang Li, Mingchuan Li, Shu Li, Shuaijie Lin, Qing Liu, Jianglai Lu, Xiaoying Luo, Lingyin Ma, Wenbo Ma, Yugang Mao, Yajun Meng, Yue Ning, Xuyang Qi, Ningchun Ren, Xiangxiang Shaheed, Nasir Shang, Changsong Shen, Guofang Sun, Wenliang Tan, Andi Tao, Yi Wang, Anqing Wang, Meng Wang, Qiuhong Wang, Shaobo Wang, Siguang Wang, Wei Wang, Xiuli Wang, Zhou Wu, Mengmeng Wu, Weihao Xia, Jingkai Xiao, Mengjiao Xiao, Xiang Xie, Pengwei Yan, Binbin Yan, Xiyu Yang, Jijun Yang, Yong Yu, Chunxu Yuan, Jumin Yuan, Ying Zhang, Dan Zhang, Minzhen Zhang, Peng Zhang, Tao Zhao, Li Zheng, Qibin Zhou, Jifang Zhou, Ning Zhou, Xiaopeng Zhou, Yong |
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low radioactive material screening and background control for the pandax-4t experiment |
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Low radioactive material screening and background control for the PandaX-4T experiment |
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Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. © The Author(s) 2022 |
abstractGer |
Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. © The Author(s) 2022 |
abstract_unstemmed |
Abstract PandaX-4T is a ton-scale dark matter direct detection experiment using a dual-phase TPC technique at the China Jinping Underground Laboratory. Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. In addition, natKr in the detector is estimated to be < 8 ppt. © The Author(s) 2022 |
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Low radioactive material screening and background control for the PandaX-4T experiment |
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Si, Lin Abdukerim, Abdusalam Bo, Zihao Chen, Wei Chen, Xun Chen, Yunhua Cheng, Chen Cheng, Yunshan Cui, Xiangyi Fan, Yingjie Fang, Deqing Fu, Changbo Fu, Mengting Geng, Lisheng Giboni, Karl Gu, Linhui Guo, Xuyuan Han, Ke He, Changda He, Jinrong Huang, Di Huang, Yanlin Huang, Zhou Hou, Ruquan Ji, Xiangdong Ju, Yonglin Li, Chenxiang Li, Mingchuan Li, Shu Li, Shuaijie Lin, Qing Liu, Jianglai Lu, Xiaoying Luo, Lingyin Ma, Wenbo Ma, Yugang Mao, Yajun Meng, Yue Ning, Xuyang Qi, Ningchun Ren, Xiangxiang Shaheed, Nasir Shang, Changsong Shen, Guofang Sun, Wenliang Tan, Andi Tao, Yi Wang, Anqing Wang, Meng Wang, Qiuhong Wang, Shaobo Wang, Siguang Wang, Wei Wang, Xiuli Wang, Zhou Wu, Mengmeng Wu, Weihao Xia, Jingkai Xiao, Mengjiao Xiao, Xiang Xie, Pengwei Yan, Binbin Yan, Xiyu Yang, Jijun Yang, Yong Yu, Chunxu Yuan, Jumin Yuan, Ying Zhang, Dan Zhang, Minzhen Zhang, Peng Zhang, Tao Zhao, Li Zheng, Qibin Zhou, Jifang Zhou, Ning Zhou, Xiaopeng Zhou, Yong |
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Si, Lin Abdukerim, Abdusalam Bo, Zihao Chen, Wei Chen, Xun Chen, Yunhua Cheng, Chen Cheng, Yunshan Cui, Xiangyi Fan, Yingjie Fang, Deqing Fu, Changbo Fu, Mengting Geng, Lisheng Giboni, Karl Gu, Linhui Guo, Xuyuan Han, Ke He, Changda He, Jinrong Huang, Di Huang, Yanlin Huang, Zhou Hou, Ruquan Ji, Xiangdong Ju, Yonglin Li, Chenxiang Li, Mingchuan Li, Shu Li, Shuaijie Lin, Qing Liu, Jianglai Lu, Xiaoying Luo, Lingyin Ma, Wenbo Ma, Yugang Mao, Yajun Meng, Yue Ning, Xuyang Qi, Ningchun Ren, Xiangxiang Shaheed, Nasir Shang, Changsong Shen, Guofang Sun, Wenliang Tan, Andi Tao, Yi Wang, Anqing Wang, Meng Wang, Qiuhong Wang, Shaobo Wang, Siguang Wang, Wei Wang, Xiuli Wang, Zhou Wu, Mengmeng Wu, Weihao Xia, Jingkai Xiao, Mengjiao Xiao, Xiang Xie, Pengwei Yan, Binbin Yan, Xiyu Yang, Jijun Yang, Yong Yu, Chunxu Yuan, Jumin Yuan, Ying Zhang, Dan Zhang, Minzhen Zhang, Peng Zhang, Tao Zhao, Li Zheng, Qibin Zhou, Jifang Zhou, Ning Zhou, Xiaopeng Zhou, Yong |
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Various ultra-low background technologies have been developed and applied to material screening for PandaX-4T, including HPGe gamma spectroscopy, ICP-MS, NAA, radon emanation measurement system, krypton assay station, and alpha detection system. Low background materials were selected to assemble the detector. Surface treatment procedures were investigated to further suppress radioactive background. Combining measured results and Monte Carlo simulation, the total material background rates of PandaX-4T in the energy region of 1–25 $ keV_{ee} $ are estimated to be (9.9 ± 1.9) × $ 10^{−3} $ mDRU for electron recoil and (2.8 ± 0.6) × $ 10^{−4} $ mDRU for nuclear recoil. 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