2015
DOI: 10.1016/j.astropartphys.2015.03.008
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Particle discrimination in TeO 2 bolometers using light detectors read out by transition edge sensors

Abstract: An active discrimination of the dominant α-background is the prerequisite for future neutrinoless double-beta decay experiments based on TeO2 bolometers. We investigate such α-particle rejection in cryogenic TeO2 bolometers by the detection of Cherenkov light. For a setup consisting of a massive TeO2 crystal (285 g) and a separate cryogenic light detector, both using transition edge sensors as temperature sensors operated at around 10 mK, we obtain an event-by-event identification of e/γand α-events. We find i… Show more

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Cited by 34 publications
(22 citation statements)
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References 34 publications
(32 reference statements)
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“…Re-scaling the light signal from 2615 to 2528 keV, we obtain DP=3.6, using one highly likely assumption that an α particle at 2528 keV will show a light signal equal than the same particle at 5304 keV ( 210 Po). This DP is the best ever achieved with large mass TeO 2 crystals (M > 7 g) and without the need for additional Neganov-Luke amplification [33,45,46], or more sophisticated TES sensors [47] or both [48].…”
Section: Heat and Light Measurementmentioning
confidence: 86%
“…Re-scaling the light signal from 2615 to 2528 keV, we obtain DP=3.6, using one highly likely assumption that an α particle at 2528 keV will show a light signal equal than the same particle at 5304 keV ( 210 Po). This DP is the best ever achieved with large mass TeO 2 crystals (M > 7 g) and without the need for additional Neganov-Luke amplification [33,45,46], or more sophisticated TES sensors [47] or both [48].…”
Section: Heat and Light Measurementmentioning
confidence: 86%
“…Although TeO 2 crystals are not scintillating the phonon-light technique could be applied via the detection of Cherenkov radiation [15]. The first experimental realization of this background suppression technique was achieved using silicon based NTL-amplified cryogenic light detectors [47] and has since been also achieved using silicon-on-sapphire based light detectors [48] and germanium-based NTL detectors [25]. The technique is currently also being considered for the future CUPID experiment [49,50].…”
Section: Neutrinoless Double Beta Decaymentioning
confidence: 99%
“…These are low radioactive contamination, large sensitive area (∼5x5 cm 2 ), ease of fabrication and operation on the scale of ∼1000 detectors and limited thermal and mechanical impact on the cryogenic apparatus hosting the experiment. While there are several promising experimental techniques [13,14,15], none of them meet all the above mentioned requirements at present.…”
Section: The Calder Projectmentioning
confidence: 99%