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Effects of the dense matter can induce the neutrino decay even if neutrinos are stable in vacuum. This is due to coherent interactions with matter which lead to energy level-splitting between the neutrino and antineutrino states and thereby…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zurab G. Berezhiani , Anna Rossi

While astrophysical observations imply that 85% of the matter content is unaccounted for, the nature of this dark matter (DM) component remains unknown. Weakly Interacting Massive Particles (WIMPs) - DM particles that interact at or below…

High Energy Astrophysical Phenomena · Physics 2025-07-22 Eliot Genton , Jeffrey Lazar , Carlos Argüelles , Gwenhaël de Wasseige

With positive signals from multiple direct detection experiments it will, in principle, be possible to measure the mass and cross sections of weakly-interacting massive particle (WIMP) dark matter. Recent work has shown that, with a…

Cosmology and Nongalactic Astrophysics · Physics 2015-06-03 Bradley J. Kavanagh , Mattia Fornasa , Anne M. Green

Annihilation of dark matter particles accumulated in the Sun would produce a flux of high-energy neutrinos whose prospects of detection in neutrino telescopes and detectors have been extensively discussed in the literature. However, for…

High Energy Physics - Phenomenology · Physics 2015-06-11 Nicolas Bernal , Justo Martin-Albo , Sergio Palomares-Ruiz

Dark matter particles gravitationally trapped inside the Sun may annihilate into Standard Model particles, producing a flux of neutrinos. The prospects of detecting these neutrinos in future multi-\kton{} neutrino detectors designed for…

High Energy Physics - Phenomenology · Physics 2015-03-19 Sanjib K. Agarwalla , Mattias Blennow , Enrique Fernandez Martinez , Olga Mena

Coherent elastic neutrino- and WIMP-nucleus interaction signatures are expected to be quite similar. This paper discusses how a next generation ton-scale dark matter detector could discover neutrino-nucleus coherent scattering, a…

High Energy Physics - Phenomenology · Physics 2011-09-07 A. J. Anderson , J. M. Conrad , E. Figueroa-Feliciano , K. Scholberg , J. Spitz

Detailed Monte-Carlo simulations were used to evaluate the performance of a liquid neon scintillation detector for dark matter and low-energy solar neutrino interactions. A maximum-likelihood event vertex fitter including PMT time…

Nuclear Experiment · Physics 2007-05-23 M. G. Boulay , A. Hime , J. Lidgard

Using the data recorded by the ANTARES neutrino telescope during 2007 and 2008, a search for high energy neutrinos coming from the direction of the Sun has been performed. The neutrino selection criteria have been chosen so as to maximize…

High Energy Physics - Experiment · Physics 2015-06-12 Guillaume Lambard

We report new values of weak-mixing angle ($\sin ^{2}\theta _{W}$)$,$ neutrino effective magnetic moment and the charge radius using the lowest-energy (to-date) solar neutrino data of pp, $^{7}$Be and pep spectra from phase-I and phase-II…

High Energy Physics - Phenomenology · Physics 2019-02-19 Amir N. Khan

We present a novel deep learning pipeline to perform a model-independent, likelihood-free search for anomalous (i.e., non-background) events in the proposed next generation multi-ton scale liquid Xenon-based direct detection experiment,…

Instrumentation and Detectors · Physics 2026-05-12 J. Aalbers , K. Abe , M. Adrover , S. Ahmed Maouloud , L. Althueser , D. W. P. Amaral , B. Andrieu , E. Angelino , D. Antón Martin , B. Antunovic , E. Aprile , M. Babicz , D. Bajpai , M. Balzer , E. Barberio , L. Baudis , M. Bazyk , N. F. Bell , L. Bellagamba , R. Biondi , Y. Biondi , A. Bismark , C. Boehm , K. Boese , R. Braun , A. Breskin , S. Brommer , A. Brown , G. Bruni , R. Budnik , C. Cai , C. Capelli , A. Chauvin , A. P. Cimental Chavez , A. P. Colijn , J. Conrad , J. J. Cuenca-García , V. D'Andrea , L. C. Daniel Garcia , M. P. Decowski , A. Deisting , C. Di Donato , P. Di Gangi , S. Diglio , M. Doerenkamp , G. Drexlin , K. Eitel , A. Elykov , R. Engel , A. D. Ferella , C. Ferrari , H. Fischer , T. Flehmke , M. Flierman , K. Fujikawa , W. Fulgione , C. Fuselli , P. Gaemers , R. Gaior , M. Galloway , F. Gao , N. Garroum , R. Giacomobono , F. Girard , R. Glade-Beucke , F. Glück , L. Grandi , J. Grigat , R. Größle , H. Guan , M. Guida , P. Gyorgy , R. Hammann , V. Hannen , S. Hansmann-Menzemer , N. Hargittai , A. Higuera , C. Hils , K. Hiraoka , L. Hoetzsch , M. Hoferichter , N. F. Hood , M. Iacovacci , Y. Itow , J. Jakob , R. S. James , F. Joerg , F. Kahlert , Y. Kaminaga , M. Kara , P. Kavrigin , S. Kazama , M. Keller , P. Kharbanda , B. Kilminster , M. Kleifges , M. Klute , M. Kobayashi , D. Koke , A. Kopec , B. von Krosigk , F. Kuger , L. LaCascio , H. Landsman , R. F. Lang , L. Levinson , I. Li , A. Li , S. Li , S. Liang , Z. Liang , Y. -T. Lin , S. Lindemann , M. Lindner , K. Liu , J. Loizeau , F. Lombardi , J. Long , J. A. M. Lopes , G. M. Lucchetti , T. Luce , Y. Ma , C. Macolino , J. Mahlstedt , B. Maier , A. Mancuso , L. Manenti , F. Marignetti , T. Marrodán Undagoitia , K. Martens , J. Masbou , E. Masson , S. Mastroianni , A. Melchiorre , J. Menéndez , M. Messina , B. Milosovic , S. Milutinovic , K. Miuchi , R. Miyata , A. Molinario , C. M. B. Monteiro , K. Morå , S. Moriyama , E. Morteau , Y. Mosbacher , J. Müller , M. Murra , J. L. Newstead , K. Ni , C. O'Hare , U. Oberlack , M. Obradovic , I. Ostrowskiy , S. Ouahada , B. Paetsch , Y. Pan , M. Pandurovic , Q. Pellegrini , R. Peres , F. Piastra , J. Pienaar , M. Pierre , G. Plante , T. R. Pollmann , L. Principe , J. Qi , K. Qiao , J. Qin , M. Rajado , D. Ramírez García , A. Ravindran , A. Razeto , L. Sanchez , P. Sanchez-Lucas , G. Sartorelli , A. Scaffidi , J. Schreiner , P. Schulte , H. Schulze Eißing , M. Schumann , A. Schwenck , A. Schwenk , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Sharma , W. Shen , S. Y. Shi , T. Shimada , H. Simgen , R. Singh , M. Solmaz , O. Stanley , M. Steidl , A. Stevens , A. Takeda , P. -L. Tan , D. Thers , T. Thümmler , F. Tönnies , F. Toschi , G. Trinchero , R. Trotta , C. D. Tunnell , P. Urquijo , M. Utoyama , K. Valerius , S. Vecchi , S. Vetter , G. Volta , D. Vorkapic , W. Wang , K. M. Weerman , C. Weinheimer , M. Weiss , D. Wenz , M. Wilson , C. Wittweg , J. Wolf , V. H. S. Wu , S. Wüstling , M. Wurm , Y. Xing , D. Xu , Z. Xu , M. Yamashita , L. Yang , J. Ye , L. Yuan , G. Zavattini , M. Zhong , K. Zuber

Heavy stable fourth generation Majorana neutrinos contribute to a small fraction of the relic density of dark matter (DM) in the Universe. Due to its relatively strong coupling to the standard model particles, it can be probed by the…

High Energy Physics - Phenomenology · Physics 2012-12-13 Yu-Feng Zhou

ANTARES is the first neutrino telescope in the sea. It consists of a three-dimensional array of 885 photomultipliers to collect the Cherenkov light induced by relativistic muons produced in CC interactions of high energy neutrinos. One of…

High Energy Astrophysical Phenomena · Physics 2015-06-04 J. D. Zornoza

A search for muon neutrinos originating from dark matter annihilations in the Sun is performed using the data recorded by the ANTARES neutrino telescope from 2007 to 2012. In order to obtain the best possible sensitivities to dark matter…

High Energy Astrophysical Phenomena · Physics 2016-06-13 ANTARES collaboration , S. Adrián-Martínez , A. Albert , M. André , G. Anton , M. Ardid , J. -J. Aubert , T. Avgitas , B. Baret , J. Barrios-Martí , S. Basa , V. Bertin , S. Biagi , R. Bormuth , M. C. Bouwhuis , R. Bruijn , J. Brunner , J. Busto , A. Capone , L. Caramete , J. Carr , S. Celli , T. Chiarusi , M. Circella , A. Coleiro , R. Coniglione , H. Costantini , P. Coyle , A. Creusot , A. Deschamps , G. De Bonis , C. Distefano , C. Donzaud , D. Dornic , D. Drouhin , T. Eberl , I. El Bojaddaini , D. Elsässer , A. Enzenhöfer , K. Fehn , I. Felis , L. A. Fusco , S. Galatà , P. Gay , S. Geißelsöder , K. Geyer , V. Giordano , A. Gleixner , H. Glotin , R. Gracia-Ruiz , K. Graf , S. Hallmann , H. van Haren , A. J. Heijboer , Y. Hello , J. J. Hernández-Rey , J. Hößl , J. Hofestädt , C. Hugon , G. Illuminati , C. W James , M. de Jong , M. Jongen , M. Kadler , O. Kalekin , U. Katz , D. Kießling , A. Kouchner , M. Kreter , I. Kreykenbohm , V. Kulikovskiy , C. Lachaud , R. Lahmann , D. Lefèver , E. Leonora , S. Loucatos , M. Marcelin , A. Margiotta , A. Marinelli , J. A. Martínez-Mora , A. Mathieu , K. Melis , T. Michael , P. Migliozzi , A. Moussa , C. Mueller , E. Nezri , G. E. Păvălaş , C. Pellegrino , C. Perrina , P. Piattelli , V. Popa , T. Pradier , C. Racca , G. Riccobene , K. Roensch , M. Saldana , D. F. E. Samtleben , A. Sánchez-Losa , M. Sanguineti , P. Sapienza , J. Schnabel , F. Schüssler , T. Seitz , C. Sieger , M. Spurio , Th. Stolarczyk , M. Taiuti , C. Tönnis , A. Trovato , M. Tselengidou , D. Turpin , B. Vallage , C. Vallée , V. Van Elewyck , D. Vivolo , S. Wagner , J. Wilms , J. D. Zornoza , J. Zúñiga

We identify the maximum cross sections probed by single-scatter ``WIMP" searches in dark matter direct detection. Due to Poisson fluctuations in scatter multiplicity, these ceilings scale logarithmically with mass for heavy dark matter and…

High Energy Physics - Phenomenology · Physics 2024-06-26 Nirmal Raj , Biprajit Mondal

Next-generation xenon detectors with multi-ton-year exposure are powerful direct probes of dark matter candidates, in particular the favorite weakly-interacting massive particles. Coupled with the features of low thresholds and backgrounds,…

High Energy Physics - Phenomenology · Physics 2019-10-09 Chung-Chun Hsieh , Lakhwinder Singh , Chih-Pan Wu , Jiunn-Wei Chen , Hsin-Chang Chi , C. -P. Liu , Mukesh K. Pandey , Henry T. Wong

The absence of a neutrino flux from self-annihilating dark matter captured in the Sun has tightly constrained some leading particle dark matter scenarios. The impact of astrophysical uncertainties on the capture process of dark matter in…

High Energy Astrophysical Phenomena · Physics 2015-09-29 Matthias Danninger , Carsten Rott

The measurement of the flux of beryllium neutrinos with the accuracy of about 10% and CNO neutrinos with the accuracy 30% will enable to find the flux of pp-neutrinos in the source with the accuracy better than 1% using the luminosity…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Kopylov , I. Orekhov , V. Petukhov , A. Solomatin , M. Arnoldov

A universal seesaw mass matrix model, which gives successful description of quark mass matrix in terms of lepton masses, yields three "sterile" neutrinos \nu^s_{i}, which compose pseudo-Dirac neutrinos \nu_{i\pm}^{ps}\simeq (\nu_{i} \pm…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yoshio Koide , Hideo Fusaoka

Dark matter direct detection experiments have become excellent low-energy neutrino detectors. We present a few novel ideas to probe Beyond the Standard Model physics from neutrinos at these experiments. First, we discuss signatures arising…

High Energy Physics - Phenomenology · Physics 2025-01-22 Gonzalo Herrera

Neutrino telescopes are looking to detect neutrinos produced by the annihilation of weakly interacting massive particle (WIMP) dark matter in the sun. The event rate depends on the dark matter density in the sun, which in turn is dictated…

High Energy Physics - Phenomenology · Physics 2010-03-31 Prateek Agrawal , Zackaria Chacko , Can Kilic , Rashmish K. Mishra
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