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Background of germanium and xenon detectors due to the elastic scattering of $^{8}B$ solar neutrinos on electrons have been calculated. The background is 4.6 \times $10^{-4}$ counts/(keV$\cdot t\cdot$y) that defines the sensitivity of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alexander A. Klimenko

Presently, there are several experimental setups dedicated to rare event searches, such as dark matter interactions or double beta decay, in the building or commissioning phases. These experiments often use large mass detectors and have…

High Energy Astrophysical Phenomena · Physics 2012-11-08 Carlos Martinez Amaya , Matteo Biassoni

Static gamma-ray detector systems that are deployed outdoors for radiological monitoring purposes experience time- and spatially-varying natural backgrounds and encounters with man-made nuisance sources. In order to be sensitive to illicit…

Instrumentation and Detectors · Physics 2023-09-11 M. S. Bandstra , N. Abgrall , R. J. Cooper , D. Hellfeld , T. H. Y. Joshi , V. Negut , B. J. Quiter , M. Salathe , R. Sankaran , Y. Kim , S. Shahkarami

We propose the use of silicon carbide (SiC) for direct detection of sub-GeV dark matter. SiC has properties similar to both silicon and diamond, but has two key advantages: (i) it is a polar semiconductor which allows sensitivity to a…

High Energy Physics - Phenomenology · Physics 2021-04-14 Sinéad M. Griffin , Yonit Hochberg , Katherine Inzani , Noah Kurinsky , Tongyan Lin , To Chin Yu

Phonon-mediated particle detectors based on single crystals and operated at millikelvin temperatures are used in rare-event experiments for neutrino physics and dark-matter searches. In general, these devices are not sensitive to the…

Providing a background discrimination tool is crucial for enhancing the sensitivity of next-generation experiments searching for neutrinoless double- beta decay. The development of high-sensitivity (< 20 eV RMS) cryogenic light detectors…

The PANDAX-4T and XENONnT experiments present indications of Coherent Elastic Neutrino Nucleus Scattering (CE$\nu$NS) from ${}^{8}$B solar neutrinos at 2.6$\sigma$ and 2.7$\sigma$, respectively. This constitutes the first observation of the…

High Energy Physics - Phenomenology · Physics 2025-08-04 Pablo Blanco-Mas , Pilar Coloma , Gonzalo Herrera , Patrick Huber , Joachim Kopp , Ian M. Shoemaker , Zahra Tabrizi

We explore the possibility that neutrinos couple to an interacting sterile sector, providing a novel portal that generalizes the heavy neutral lepton portal to a composite setting. For a low confinement scale, high-energy neutrino beams can…

High Energy Physics - Phenomenology · Physics 2026-04-17 Matteo Borrello , Marco Costa , Diego Redigolo , Michele Tammaro

Silicon Carbide (SiC) demonstrates significant potential for high-energy particle detection in complex radiation environments due to its exceptional radiation resistance, excellent environmental adaptability, and fast response time.…

Instrumentation and Detectors · Physics 2025-04-04 Zaiyi. Li , Xiyuan. Zhang , Congcong. Wang , Haolan. Qu , Jiaxiang. Chen , Peilian. Liu , Suyu. Xiao , Xinbo. Zou , Hai. Lu , Xin. Shi

Neutrinoless double beta decay searches play a major role in determining neutrino properties, in particular the Majorana or Dirac nature of the neutrino and the absolute scale of the neutrino mass. The consequences of these searches go…

The unique electrical and material properties of 4H-silicon-carbide (4H-SiC) make it a promising candidate material for high rate particle detectors. In contrast to the ubiquitously used silicon (Si), 4H-SiC offers a higher carrier…

The \MJ\ Collaboration is operating an array of high purity Ge detectors to search for neutrinoless double-beta decay in $^{76}$Ge. The \MJ\ \DEM\ comprises 44.1~kg of Ge detectors (29.7 kg enriched in $^{76}$Ge) split between two modules…

Nuclear Experiment · Physics 2018-04-04 C. E. Aalseth , N. Abgrall , E. Aguayo , S. I. Alvis , M. Amman , I. J. Arnquist , F. T. Avignone , H. O. Back , A. S. Barabash , P. S. Barbeau , C. J. Barton , P. J. Barton , F. E. Bertrand , T. Bode , B. Bos , M. Boswell , R. L. Brodzinski , A. W. Bradley , V. Brudanin , M. Busch , M. Buuck , A. S. Caldwell , T. S. Caldwell , Y-D. Chan , C. D. Christofferson , P. -H. Chu , J. I. Collar , D. C. Combs , R. J. Cooper , C. Cuesta , J. A. Detwiler , P. J. Doe , J. A. Dunmore , Yu. Efremenko , H. Ejiri , S. R. Elliott , J. E. Fast , P. Finnerty , F. M. Fraenkle , Z. Fu , B. K. Fujikawa , E. Fuller , A. Galindo-Uribarri , V. M. Gehman , T. Gilliss , G. K. Giovanetti , J. Goett , M. P. Green , J. Gruszko , I. S. Guinn , V. E. Guiseppe , A. L. Hallin , C. R. Haufe , L. Hehn , R. Henning , E. W. Hoppe , T. W. Hossbach , M. A. Howe , B. R. Jasinski , R. A. Johnson , K. J. Keeter , J. D. Kephart , M. F. Kidd , A. Knecht , S. I. Konovalov , R. T. Kouzes , K. T. Lesko , B. D. LaFerriere , J. Leon , L. E. Leviner , J. C. Loach , A. M. Lopez , P. N. Luke , J. MacMullin , S. MacMullin , M. G. Marino , R. D. Martin , R. Massarczyk , A. B. McDonald , D. -M. Mei , S. J. Meijer , J. H. Merriman , S. Mertens , H. S. Miley , M. L. Miller , J. Myslik , J. L. Orrell , C. O'Shaughnessy , G. Othman , N. R. Overman , W. Pettus , D. G. Phillips , A. W. P. Poon , G. Perumpilly , K. Pushkin , D. C. Radford , J. Rager , J. H. Reeves , A. L. Reine , K. Rielage , R. G. H. Robertson , M. C. Ronquest , N. W. Ruof , A. G. Schubert , B. Shanks , M. Shirchenko , K. J. Snavely , N. Snyder , D. Steele , A. M. Suriano , D. Tedeschi , W. Tornow , J. E. Trimble , R. L. Varner , S. Vasilyev , K. Vetter , K. Vorren , B. R. White , J. F. Wilkerson , C. Wiseman , W. Xu , E. Yakushev , H. Yaver , A. R. Young , C. -H. Yu , V. Yumatov , I. Zhitnikov , B. X. Zhu , S. Zimmermann

Dark Matter In CCDs (DAMIC) is a silicon detector apparatus used primarily for searching for low-mass dark matter using the silicon bulk of Charge-Coupled Devices (CCDs) as targets. The silicon target within each CCD is…

Instrumentation and Detectors · Physics 2020-03-09 Steven Juhyung Lee , Ben Kilminster , Anna Macchiolo

To cope with environments with high levels of radiation, non-silicon semiconductors such as silicon carbide detectors are being proposed for instrumentation. 4H-SiC diodes for radiation detection have been fabricated in the IMB-CNM Clean…

In the commissioning phase of the DANCE project (Detector for Advanced Neutron Capture Experiments) measurements have been performed with special emphasis on the identification and suppression of possible backgrounds for the planned (n,g)…

We have developed a neutrino detector with threshold energies from ~0.115 to 105 MeV in a clean detection mode almost completely void of accidental backgrounds. It was initially developed for the NASA $\nu$SOL project to put a solar…

SoLid, located at SCK-CEN in Mol, Belgium, is a reactor antineutrino experiment at a very short baseline of 5.5 -- 10m aiming at the search for sterile neutrinos and for high precision measurement of the neutrino energy spectrum of…

Instrumentation and Detectors · Physics 2019-05-03 Lukas On Arnold

Both active and sterile sub-eV neutrinos can form the cosmic neutrino background in the early Universe. We consider the beta-decaying (e.g., $^3$H) and EC-decaying (e.g., $^{163}$Ho) nuclei as the promising targets to capture relic…

Cosmology and Nongalactic Astrophysics · Physics 2016-06-16 Yu-Feng Li

The high-luminosity operation of the Tracker in the Compact Muon Solenid (CMS) detector at the Large Hadron Collider (LHC) experiment calls for the development of silicon-based sensors. This involves implementation of AC-coupling to…