2018
DOI: 10.1088/1748-0221/13/02/c02001
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Radon background in liquid xenon detectors

Abstract: The radioactive daughters isotope of 222 Rn are one of the highest risk contaminants in liquid xenon detectors aiming for a small signal rate. The noble gas is permanently emanated from the detector surfaces and mixed with the xenon target. Because of its long half-life 222 Rn is homogeneously distributed in the target and its subsequent decays can mimic signal events. Since no shielding is possible this background source can be the dominant one in future large scale experiments. This article provides an ove… Show more

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Cited by 6 publications
(3 citation statements)
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“…1 H NMRs were acquired on 300 MHz and 500 MHz spectrometers and referenced to the internal solvent signals (7.26 ppm in CDCl 3 or 3.33 ppm in CD 3 OD). 13 C NMRs were acquired on 75 MHz and 125 MHz spectrometers referenced to the internal solvent signals (central peak 77.00 ppm in CDCl 3 or 45.00 ppm in CD 3 OD). NMR data are reported as follows: chemical shift (in ppm, δ ), integration, multiplicity (s = singlet, d = doublet, t = triplet, q = quartet, m = multiplet, br = broad), coupling constant (in Hz).…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…1 H NMRs were acquired on 300 MHz and 500 MHz spectrometers and referenced to the internal solvent signals (7.26 ppm in CDCl 3 or 3.33 ppm in CD 3 OD). 13 C NMRs were acquired on 75 MHz and 125 MHz spectrometers referenced to the internal solvent signals (central peak 77.00 ppm in CDCl 3 or 45.00 ppm in CD 3 OD). NMR data are reported as follows: chemical shift (in ppm, δ ), integration, multiplicity (s = singlet, d = doublet, t = triplet, q = quartet, m = multiplet, br = broad), coupling constant (in Hz).…”
Section: Methodsmentioning
confidence: 99%
“…Well-motivated theoretical models involving light neutrino exchange predict that 0νβ β could be observed with any lifetime beyond this limit [8][9][10] , given present knowledge of neutrino masses and mixing angles. Observing such a rare process above experimental background from sources such as detector material gamma rays 11 , dissolved radioisotopes 12,13 , neutron captures 14 , and others is a formidable experimental challenge, requiring deep underground detectors, exquisite radio-purity [15][16][17] , and extremely selective signal identification and background rejection methods.…”
Section: Introductionmentioning
confidence: 99%
“…Radon can be removed from gases (including air) using purification columns filled with adsorbers, such as charcoal, typically operated at cryogenic temperatures [4,5]. Radon can also be removed via nitrogen gas stripping [4,6] or via liquid distillation [7]. Because of these reasons, radio-assay measurements of detector components via gamma-ray spectroscopy or mass spectrometry techniques prior to detector installation are of limited use to constrain radon-induced backgrounds.…”
Section: Introductionmentioning
confidence: 99%