English
Related papers

Related papers: The CUORE experiment at LNGS

200 papers

Large-mass bolometers are used in particle physics experiments to search for rare processes. The energy threshold of such detectors plays a critical role in their capability to search for dark matter interactions and rare nuclear decays. We…

Instrumentation and Methods for Astrophysics · Physics 2015-03-17 Sergio Di Domizio , Filippo Orio , Marco Vignati

The LUCE (LUtetium sCintillation Experiment) project will search for the 176Lu electron capture based on a milli-Kelvin calorimetric approach. This decay is of special interest in the field of nuclear structure, with implications for the…

The Deep Underground Neutrino Experiment (DUNE) is a leading-edge experiment designed to perform neutrino science and proton decay searches. In particular, the far detector will consist of four 10-kton Liquid Argon (LAr) Time Projection…

Instrumentation and Detectors · Physics 2020-08-26 Chiara Lastoria

The international project ``Microcalorimeter Arrays for a Rhenium Experiment'' (MARE) aims at the direct and calorimetric measurement of the electron neutrino mass with sub-electronvolt sensitivity. Calorimetric neutrino mass experiments…

High Energy Physics - Experiment · Physics 2019-08-13 A. Nucciotti

The cryogenic phonon scintillating bolometer is a promising and extremely attractive option to search for the nuclide neutrinoless double beta decay. In this paper, a pre-study of bolometer based on Li2MoO4 (LMO) crystal is presented, in…

Instrumentation and Detectors · Physics 2025-05-06 Deyong Duan , Mingxuan Xue , Kangkang Zhao , Taiyuan Liu , Haiping Peng , Jiaxuan Cao , Long Ma , Liang Chen , Hui Yuan , Qing Lin , Zizong Xua , Xiaolian Wang

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…

We report the development of a CaMoO4 crystal low temperature detector for the AMoRE neutrinoless double beta decay (0{\nu}\b{eta}\b{eta}) search experiment. The prototype detector cell was composed of a 216 g CaMoO4 crystal and a metallic…

The CUPID-0 detector hosted at the Laboratori Nazionali del Gran Sasso, Italy, is the first large array of enriched scintillating cryogenic detectors for the investigation of $^{82}$Se neutrinoless double-beta decay (0$\nu\beta\beta$).…

Neutrinoless double beta decay (0nubb) is one of the most sensitive probes for physics beyond the Standard Model, providing unique information on the nature of neutrinos. In this paper we review the status and outlook for bolometric 0nubb…

Nuclear Experiment · Physics 2014-04-18 D. R. Artusa , F. T. Avignone , O. Azzolini , M. Balata , T. I. Banks , G. Bari , J. Beeman , F. Bellini , A. Bersani , M. Biassoni , C. Brofferio , C. Bucci , X. Z. Cai , A. Camacho , L. Canonica , X. G. Cao , S. Capelli , L. Carbone , L. Cardani , M. Carrettoni , N. Casali , D. Chiesa , N. Chott , M. Clemenza , C. Cosmelli , O. Cremonesi , R. J. Creswick , I. Dafinei , A. Dally , V. Datskov , A. De Biasi , M. M. Deninno , S. Di Domizio , M. L. di Vacri , L. Ejzak , D. Q. Fang , H. A. Farach , M. Faverzani , G. Fernandes , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , B. K. Fujikawa , A. Giachero , L. Gironi , A. Giuliani , J. Goett , P. Gorla , C. Gotti , T. D. Gutierrez , E. E. Haller , K. Han , K. M. Heeger , R. Hennings-Yeomans , H. Z. Huang , R. Kadel , K. Kazkaz , G. Keppel , Yu. G. Kolomensky , Y. L. Li , C. Ligi , X. Liu , Y. G. Ma , C. Maiano , M. Maino , M. Martinez , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , T. Napolitano , S. Nisi , C. Nones , E. B. Norman , A. Nucciotti , T. O'Donnell , F. Orio , D. Orlandi , J. L. Ouellet , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , G. Pessina , V. Pettinacci , G. Piperno , C. Pira , S. Pirro , E. Previtali , V. Rampazzo , C. Rosenfeld , C. Rusconi , E. Sala , S. Sangiorgio , N. D. Scielzo , M. Sisti , A. R. Smith , L. Taffarello , M. Tenconi , F. Terranova , W. D. Tian , C. Tomei , S. Trentalange , G. Ventura , M. Vignati , B. S. Wang , H. W. Wang , L. Wielgus , J. Wilson , L. A. Winslow , T. Wise , A. Woodcraft , L. Zanotti , C. Zarra , B. X. Zhu , S. Zucchelli

The RICOCHET reactor neutrino observatory is planned to be installed at the Laue Langevin Institute (ILL) starting mid-2022. Its scientific goal is to perform a low-energy and high precision measurement of the coherent elastic…

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$_{2}$…

The Deep Underground Neutrino Experiment (DUNE) is a dual-site experiment for long baseline neutrino oscillation studies, and for neutrino astrophysics and nucleon decay searches. DUNE will comprise four 10 kton fiducial liquid argon…

Instrumentation and Detectors · Physics 2019-10-23 C. Cuesta

The Cooling Storage Ring (CSR) External-target Experiment (CEE) at the Heavy Ion Research Facility in Lanzhou (HIRFL), China, is the first multi-purpose nuclear physics experimental device to operate in the Giga electron-volt (GeV) energy…

Instrumentation and Detectors · Physics 2023-04-07 D. Hu , X. Wang , M. Shao , Y. Zhou , S. Ye , L. Zhao , Y. Sun , J. Lu , H. Xu

We report a study on the background of the Advanced Molybdenum-Based Rare process Experiment (AMoRE), a search for neutrinoless double beta decay (\znbb) of $^{100}$Mo. The pilot stage of the experiment was conducted using $\sim$1.9 kg of…

The IceCube neutrino observatory in operation at the South Pole, Antarctica, comprises three distinct components: a large buried array for ultrahigh energy neutrino detection, a surface air shower array, and a new buried component called…

Instrumentation and Methods for Astrophysics · Physics 2012-08-27 The IceCube Collaboration

Cryogenic macro-calorimeters instrumented with NTD thermistors have been developed for several decades. The choice of the optimal bias current is crucial for a proper operation of these detectors, both in terms of energy resolution and…