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Related papers: Scintillating double beta decay bolometers

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Fast timing detectors are an essential element in the experimental setup for time-of-flight (ToF) mass measurements of unstable nuclei. We have upgraded the scintillator detectors used in experiments at the National Superconducting…

The LUMINEU project aims at performing a demonstrator underground experiment searching for the neutrinoless double beta decay of the isotope $^{100}$Mo embedded in zinc molybdate (ZnMoO$_4$) scintillating bolometers. In this context, a zinc…

Scintillation properties of the new Tl2LaCl5: xCe3+ where x = 0, 0.5, 1 and 10 mole % (TLC: Ce3+) single crystals are presented. Two zones vertical Bridgman technique is used for the growth of this scintillation material. High Z-number (79)…

Materials Science · Physics 2017-04-05 H. J. Kim , Gul Rooh , Sunghwan Kim

An active discrimination of the dominant $\alpha$-background is the prerequisite for future neutrinoless double-beta decay experiments based on TeO$_{2}$ bolometers. We investigate such $\alpha$-particle rejection in cryogenic TeO$_{2}$…

SNO+ will search for neutrinoless double beta decay by loading 780 tonnes of linear alkylbenzene liquid scintillator with O(tonne) of neodymium. Using natural Nd at 0.1% loading will provide 43.7 kg of 150Nd given its 5.6% abundance and…

Instrumentation and Detectors · Physics 2019-08-14 J. Hartnell

For the first time a PbWO4 crystal was grown using ancient Roman lead and it was run as a cryogenic detector. Thanks to the simultaneous and independent read-out of heat and scintillation light, the detector was able to discriminate…

We present the performances of two 92% enriched $^{130}$TeO$_2$ crystals operated as thermal bolometers in view of a next generation experiment to search for neutrinoless double beta decay of $^{130}$Te. The crystals, 435 g each, show an…

A scintillating bolometer based on a large cubic Li$_{2}$$^{100}$MoO$_4$ crystal (45 mm side) and a Ge wafer (scintillation detector) has been operated in the CROSS cryogenic facility at the Canfranc underground laboratory in Spain. The…

Instrumentation and Detectors · Physics 2021-03-24 The CUPID Interest Group , A. Armatol , E. Armengaud , W. Armstrong , C. Augier , F. T. Avignone , O. Azzolini , I. C. Bandac , A. S. Barabash , G. Bari , A. Barresi , D. Baudin , F. Bellini , G. Benato , M. Beretta , L. Bergé , Ch. Bourgeois , M. Biassoni , J. Billard , V. Boldrini , A. Branca , C. Brofferio , C. Bucci , J. M. Calvo-Mozota , J. Camilleri , A. Candela , S. Capelli , L. Cappelli , L. Cardani , P. Carniti , N. Casali , A. Cazes , E. Celi , C. Chang , M. Chapellier , A. Charrier , D. Chiesa , M. Clemenza , I. Colantoni , F. Collamati , S. Copello , F. Cova , O. Cremonesi , R. J. Creswick , A. Cruciani , A. D'Addabbo , G. D'Imperio , I. Dafinei , F. A. Danevich , M. de Combarieu , M. De Deo , M. De Jesus , P. de Marcillac , S. Dell'Oro , S. Di Domizio , V. Dompe , A. Drobizhev , L. Dumoulin , G. Fantini , M. Fasoli , M. Faverzani , E. Ferri , F. Ferri , F. Ferroni , E. Figueroa-Feliciano , J. Formaggio , A. Franceschi , C. Fu , S. Fu , B. K. Fujikawa , J. Gascon , A. Giachero , L. Gironi , A. Giuliani , P. Gorla , C. Gotti , P. Gras , M. Gros , E. Guerard , T. D. Gutierrez , K. Han , E. V. Hansen , K. M. Heeger , D. L. Helis , H. Z. Huang , R. G. Huang , A. Ianni , L. Imbert , J. Johnston , A. Juillard , G. Karapetrov , G. Keppel , H. Khalife , V. V. Kobychev , Yu. G. Kolomensky , S. I. Konovalov , Y. Liu , P. Loaiza , L. Ma , M. Madhukuttan , F. Mancarella , R. Mariam , L. Marini , S. Marnieros , M. Martinez , R. H. Maruyama , B. Mauri , D. Mayer , Y. Mei , S. Milana , D. Misiak , T. Napolitano , M. Nastasi , X. -F. Navick , J. Nikkel , R. Nipoti , S. Nisi , C. Nones , E. B. Norman , V. Novosad , I. Nutini , T. O'Donnell , G. Olivier , E. Olivieri , C. Oriol , J. L. Ouellet , S. Pagan , C. Pagliarone , L. Pagnanini , P. Pari , L. Pattavina , B. Paul , M. Pavan , H. Peng , G. Pessina , V. Pettinacci , C. Pira , S. Pirro , D. V. Poda , T. Polakovic , O. G. Polischuk , S. Pozzi , E. Previtali , A. Puiu , A. Ressa , D. Reynet , R. Rizzoli , C. Rosenfeld , V. Sanglard , J. A. Scarpaci , B. Schmidt , V. Sharma , V. N. Shlegel , V. Singh , M. Sisti , D. Speller , P. T. Surukuchi , L. Taffarello , O. Tellier , C. Tomei , V. I. Tretyak , A. Tsymbaliuk , A. Vedda , M. Velazquez , K. J. Vetter , S. L. Wagaarachchi , G. Wang , L. Wang , B. Welliver , J. Wilson , K. Wilson , L. A. Winslow , M. Xue , L. Yan , J. Yang , V. Yefremenko , V. I. Yumatov , M. M. Zarytskyy , J. Zhang , A. S. Zolotarova , S. Zucchelli

We present the performances of Li-based compounds used as scintillating bolometer for rare decay studies such as double-beta decay and direct dark matter investigations. The compounds are tested in a dilution refrigerator installed in the…

Instrumentation and Detectors · Physics 2014-03-12 L. Pattavina

The scintillation decay time constant of a ZnWO$_4$ crystal irradiated with $\alpha$-particles from $^{241}$Am was precisely investigated, and was found to depend on the incident direction of the $\alpha$-particles on the crystal. The…

Instrumentation and Detectors · Physics 2022-01-27 M. Shibata , H. Sekiya , K. Ichimura

Nuclear and high energy physics research has a need for new, high performance scintillators with high light yields; high densities, fast decay times, and are radiation hard. In this paper we present crystal growth and results from 16-mm…

Instrumentation and Detectors · Physics 2021-05-03 R. Hawrami , E. Ariesanti , A. Burger , H. Parkhe

Possibilities to search for double beta decay of alpha/beta unstable nuclei, many of which have higher energy release than "conventional" (beta stable) double beta decay candidates, are discussed. First experimental half-life limits on…

Nuclear Experiment · Physics 2009-11-10 V. I. Tretyak , F. A. Danevich , S. S. Nagorny , Yu. G. Zdesenko

We present measurements of nonproportionality in the scintillation light yield of bismuth germanate (BGO) for gamma-rays with energies between 6 keV and 662 keV. The scintillation light was read out by avalanche photodiodes (APDs) with both…

Instrumentation and Detectors · Physics 2015-05-04 T. R. Gentile , M. J. Bales , H. Breuer , T. E. Chupp , K. J. Coakley , R. L. Cooper , J. S. Nico , B. O'Neill

A scintillating fiber array measurement system for gross beta is developed to achieve real-time monitoring of radioactivity in drinking water. The detector consists of 1,096 scintillating fibers, both sides of the fibers connect to a…

Instrumentation and Detectors · Physics 2017-07-20 Wenhui Lu , Hongchang Yi , Tongqing Liu , Zhi Zeng , Junli Li , Hui Zhang , Hao Ma

Double beta plus decay is a rare nuclear disintegration process. Difficulties in its measurement arise from suppressed decay probabilities, experimentally challenging decay signatures and low natural abundances of suitable candidate nuclei.…

Liquid-scintillator-based detectors are a robust technology that scales well to large volumes. For this reason, they are attractive for experiments searching for neutrinoless double-beta decay. A combination of improved photo-detection…

Instrumentation and Detectors · Physics 2013-07-12 Lindley Winslow

The possible use of a Spherical Proportional Counter for the search of neutrinoless double beta decay is investigated in the R2D2 R&D project. Dual charge and scintillation light readout may improve the detector performance. Tests were…

CUORE, an array of 988 TeO$_2$ bolometers, is about to be one of the most sensitive experiments searching for neutrinoless double-beta decay. Its sensitivity could be further improved by removing the background from $\alpha$ radioactivity.…

Next-generation large-scale neutrino detectors, from Eos, at the 1 tonne scale, to Theia, at the 10s-of-ktonne scale, will utilize differences in both the scintillation and Cherenkov light emission for different particle species to perform…

High Energy Physics - Experiment · Physics 2023-12-04 E. J. Callaghan , T. Kaptanoglu , M. Smiley , M. Yeh , G. D. Orebi Gann

The scintillation characteristics of 1 g undoped CsI crystal were studied by directly coupling two silicon photomultipliers(SiPMs) over a temperature range from room temperature to 86 K. The scintillation decay time and light output were…

Instrumentation and Detectors · Physics 2025-08-01 W. K. Kim , H. Y. Lee , K. W. Kim , Y. J. Ko , J. A. Jeon , H. J. Kim , H. S. Lee
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