DARKSIDE()
- Proposed: Nov 13, 2009,
- Approved: Dec 1, 2009,
- Started: 2013,
- Completed: 9999
A leading candidate explanation, motivated by supersymmetry theory, is that dark matter is comprised of as yet undiscovered Weakly Interacting Massive Particles (WIMPs) formed in the early universe and subsequently gravitationally clustered in association with baryonic matter. WIMPs could in principle be detected in terrestrial experiments through their collisions with ordinary nuclei, giving observable low-energy (<100 keV) nuclear recoils. The predicted low collision rates require ultra-low background detectors with large (0.1–10 ton) target masses, located in deep underground sites to eliminate neutron background from cosmic ray muons.
Among a number of developing detector technologies, two-phase liquid argon time projection chambers (LAr TPCs), which detect scintillation light and ionization generated by recoiling nuclei, are particularly promising. The signal/background discrimination power and the attainable precision for determining 3-D event positions have been demonstrated in published results from members of the present collaboration.
We propose to develop and operate a series of new liquid argon detectors for WIMP detection. The first detector in the program intended to make physics measurements will be DarkSide-50 (DS-50), with 50kg active mass, which is scheduled to begin commissioning at Gran Sasso Underground Laboratory at the beginning of 2013. The program is intended to progress to multi-ton detectors with high sensitivity for WIMP detection.
Detectors of the DarkSide program will use several innovative techniques to positively identify Dark Matter signals and to understand and suppress background. These techniques include the use of argon from underground rather than atmospheric sources, to drastically lower the radioactive 39-Ar background; an active neutron veto to strongly suppress neutron backgrounds; and comprehensive measures to control background sources in the detector and photosensors.
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- Published in:
- JINST 19 (2024) 06, C06003
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- PoS EPS-HEP2023 (2024) 110
- Contribution to:
- , 110
- EPS-HEP2023
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- PoS TAUP2023 (2024) 079
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- , 079
- TAUP 2023
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- JINST 19 (2024) 05, P05057
- e-Print:
- 2311.18647 [hep-ex]
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- AIP Conf.Proc. 2908 (2023) 1, 090003
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- Phys.Rev.D 110 (2024) 10, 102006
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- 2307.07249 [hep-ex]
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- SciPost Phys.Proc. 12 (2023) 022
- Contribution to:
- , 022
- IDM2022
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- Eur.Phys.J.C 83 (2023) 322
- e-Print:
- 2302.01830 [hep-ex]
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- EPJ Web Conf. 280 (2023) 06003
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- Published in:•
- JINST 18 (2023) 03, C03018
- e-Print:
- 2212.02299 [physics.ins-det]
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- JINST 18 (2023) 03, C03024
- e-Print:
- 2212.02296 [physics.ins-det]
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- Nuovo Cim.C 45 (2022) 5, 138
- Contribution to:
- , 138
- SIF 2021
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- Phys.Rev.Lett. 130 (2023) 10, 10
- e-Print:
- 2207.11968 [hep-ex]
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- Phys.Rev.Lett. 130 (2023) 10, 10
- e-Print:
- 2207.11967 [hep-ex]
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- PoS EPS-HEP2021 (2022) 169
- Contribution to:
- , 169
- EPS-HEP2021
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- Acta Phys.Polon.Supp. 15 (2022) 3, 29
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- J.Phys.Conf.Ser. 2156 (2021) 1, 012236,
- J.Phys.Conf.Ser. 2156 (2021) 1, 012236
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- e-Print:
- 2112.04990 [physics.ins-det]
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- Astropart.Phys. 140 (2022) 102704
- e-Print:
- 2107.08015 [physics.ins-det]
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- Phys.Rev.D 104 (2021) 8, 082005
- e-Print:
- 2107.08087 [physics.ins-det]
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- Eur.Phys.J.C 81 (2021) 4, 359
- e-Print:
- 2101.08686 [physics.ins-det]
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- Nuovo Cim.C 44 (2021) 1, 11
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- EPJ Web Conf. 251 (2021) 03029
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- Nuovo Cim.C 45 (2021) 1, 21
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- , 21
- SoUP2021
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- Nucl.Instrum.Meth.A 980 (2020) 164487
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