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In order to carry out research in the field of possible existence of a sterile neutrino the laboratory based on SM-3 reactor (Dimitrovgrad, Russia) was created to search for oscillations of reactor antineutrino. The prototype of a…

Probing neutrinoless double beta decay is one of the primary goals for SNO+, SNOLAB's multi-purpose neutrino detector. In order to achieve this goal the SNO detector has been adapted so that it can be filled with Te-loaded liquid…

Instrumentation and Detectors · Physics 2015-05-04 Evelina Arushanova , Ashley R. Back

We analyze the cumulative data from the latest SNO, KamLAND and other solar neutrino experiments in the standard scenario of three oscillating active neutrinos. We determine the solar neutrino oscillation parameters and obtain new bounds on…

High Energy Physics - Phenomenology · Physics 2009-09-15 A. B. Balantekin , V. Barger , D. Marfatia , S. Pakvasa , H. Yuksel

In the recent years important discoveries in the field of low energy neutrino physics (E$_\nu$ in the $\approx$ MeV range) have been achieved. Results of the solar neutrino experiment SNO show clearly flavor transitions from $\nu_e$ to…

High Energy Physics - Phenomenology · Physics 2009-11-10 Lothar Oberauer

After a logically clear and simple solution of the solar neutrino problem on the basis of the hypothesis about the existence of a new interaction involving electron neutrinos and nucleons, the question arose about the origin of the…

High Energy Physics - Phenomenology · Physics 2019-12-25 L. M. Slad

In the context of three-neutrino oscillations, we study the possibility of using antineutrinos from nuclear reactors to explore the 10^{-4} {\rm eV^2} < \ms \ltap 8\times 10^{-4} {\rm eV^2} region of the LMA MSW solution of the solar…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. T. Petcov , M. Piai

Determination of neutrino mass ordering and precision measurement of neutrino oscillation parameters are the foremost goals of the JUNO experiment. Here, we explore the effects of scalar non-standard interactions (sNSI) on the electron…

High Energy Physics - Phenomenology · Physics 2025-07-16 Aman Gupta , Debasish Majumdar , Suprabh Prakash

After the KamLAND results, the remaining important targets in neutrino experiments are to measure still unknown 3 basic parameters; absolute neutrino mass scale, CP violation phase $\delta_{CP}$ and last mixing angle $\theta_{13}$. The…

High Energy Physics - Experiment · Physics 2017-08-23 F. Suekane , K. Inoue , T. Araki , K. Jongok

The Sudbury Neutrino Observatory (SNO) was a heavy water Cerenkov detector designed to solve the long-standing ``solar neutrino problem''; a discrepancy between the measured and predicted flux of electron-flavour solar neutrinos. SNO…

High Energy Physics - Experiment · Physics 2009-06-01 Ryan Martin

We give an alternative description of the data produced in the KamLAND experiment, assuming the existence of a natural nuclear reactor on the boundary of the liquid and solid phases of the Earth's core. Analyzing the uncertainty of…

The SNO+ experiment is located 2 km underground at SNOLAB in Sudbury, Canada. A low background search for neutrinoless double beta ($0\nu\beta\beta$) decay will be conducted using 780 tonnes of liquid scintillator loaded with 3.9 tonnes of…

Instrumentation and Detectors · Physics 2021-08-27 SNO+ Collaboration , : , V. Albanese , R. Alves , M. R. Anderson , S. Andringa , L. Anselmo , E. Arushanova , S. Asahi , M. Askins , D. J. Auty , A. R. Back , S. Back , F. Barão , Z. Barnard , A. Barr , N. Barros , D. Bartlett , R. Bayes , C. Beaudoin , E. W. Beier , G. Berardi , A. Bialek , S. D. Biller , E. Blucher , R. Bonventre , M. Boulay , D. Braid , E. Caden , E. J. Callaghan , J. Caravaca , J. Carvalho , L. Cavalli , D. Chauhan , M. Chen , O. Chkvorets , K. J. Clark , B. Cleveland , C. Connors , D. Cookman , I. T. Coulter , M. A. Cox , D. Cressy , X. Dai , C. Darrach , B. Davis-Purcell , C. Deluce , M. M. Depatie , F. Descamps , F. Di Lodovico , J. Dittmer , A. Doxtator , N. Duhaime , F. Duncan , J. Dunger , A. D. Earle , D. Fabris , E. Falk , A. Farrugia , N. Fatemighomi , C. Felber , V. Fischer , E. Fletcher , R. Ford , K. Frankiewicz , N. Gagnon , A. Gaur , J. Gauthier , A. Gibson-Foster , K. Gilje , O. I. González-Reina , D. Gooding , P. Gorel , K. Graham , C. Grant , J. Grove , S. Grullon , E. Guillian , S. Hall , A. L. Hallin , D. Hallman , S. Hans , J. Hartnell , P. Harvey , M. Hedayatipour , W. J. Heintzelman , J. Heise , R. L. Helmer , B. Hodak , M. Hodak , M. Hood , D. Horne , B. Hreljac , J. Hu , S. M. A. Hussain , T. Iida , A. S. Inácio , C. M. Jackson , N. A. Jelley , C. J. Jillings , C. Jones , P. G. Jones , K. Kamdin , T. Kaptanoglu , J. Kaspar , K. Keeter , C. Kefelian , P. Khaghani , L. Kippenbrock , J. R. Klein , R. Knapik , J. Kofron , L. L. Kormos , S. Korte , B. Krar , C. Kraus , C. B. Krauss , T. Kroupová , K. Labe , F. Lafleur , I. Lam , C. Lan , B. J. Land , R. Lane , S. Langrock , P. Larochelle , S. Larose , A. LaTorre , I. Lawson , L. Lebanowski , G. M. Lefeuvre , E. J. Leming , A. Li , O. Li , J. Lidgard , B. Liggins , P. Liimatainen , Y. H. Lin , X. Liu , Y. Liu , V. Lozza , M. Luo , S. Maguire , A. Maio , K. Majumdar , S. Manecki , J. Maneira , R. D. Martin , E. Marzec , A. Mastbaum , A. Mathewson , N. McCauley , A. B. McDonald , K. McFarlane , P. Mekarski , M. Meyer , C. Miller , C. Mills , M. Mlejnek , E. Mony , B. Morissette , I. Morton-Blake , M. J. Mottram , S. Nae , M. Nirkko , L. J. Nolan , V. M. Novikov , H. M. O'Keeffe , E. O'Sullivan , G. D. Orebi Gann , M. J. Parnell , J. Paton , S. J. M. Peeters , T. Pershing , Z. Petriw , J. Petzoldt , L. Pickard , D. Pracsovics , G. Prior , J. C. Prouty , S. Quirk , S. Read , A. Reichold , S. Riccetto , R. Richardson , M. Rigan , I. Ritchie , A. Robertson , B. C. Robertson , J. Rose , R. Rosero , P. M. Rost , J. Rumleskie , M. A. Schumaker , M. H. Schwendener , D. Scislowski , J. Secrest , M. Seddighin , L. Segui , S. Seibert , I. Semenec , F. Shaker , T. Shantz , M. K. Sharma , T. M. Shokair , L. Sibley , J. R. Sinclair , K. Singh , P. Skensved , M. Smiley , T. Sonley , A. Sörensen , M. St-Amant , R. Stainforth , S. Stankiewicz , M. Strait , M. I. Stringer , A. Stripay , R. Svoboda , S. Tacchino , B. Tam , C. Tanguay , J. Tatar , L. Tian , N. Tolich , J. Tseng , H. W. C. Tseung , E. Turner , R. Van Berg , E. Vázquez-Jáuregui , J. G. C. Veinot , C. J. Virtue , B. von Krosigk , J. M. G. Walker , M. Walker , J. Wallig , S. C. Walton , J. Wang , M. Ward , O. Wasalski , J. Waterfield , J. J. Weigand , R. F. White , J. R. Wilson , T. J. Winchester , P. Woosaree , A. Wright , J. P. Yanez , M. Yeh , T. Zhang , Y. Zhang , T. Zhao , K. Zuber , A. Zummo

The SNO+ experiment is located at SNOLAB in Sudbury, Ontario, Canada. It will employ 780 tonnes of liquid scintillator loaded, in its initial phase, with 1.3 tonnes of $^{130}$Te (0.5% by mass) for a low-background and high-isotope-mass…

Instrumentation and Detectors · Physics 2019-08-14 Erica Caden

Antineutrinos produced at nuclear reactors constitute a severe source of background for the detection of geoneutrinos, which bring to the Earth's surface information about natural radioactivity in the whole planet. In this framework we…

Instrumentation and Detectors · Physics 2015-06-23 Marica Baldoncini , Ivan Callegari , Giovanni Fiorentini , Fabio Mantovani , Barbara Ricci , Virginia Strati , Gerti Xhixha

The main physics goal of the SNO+ experiment is the search for neutrinoless double-beta decay (0$\nu\beta\beta$), a rare process which if detected, will prove the Majorana nature of neutrinos and provide information on the absolute scale of…

Instrumentation and Detectors · Physics 2017-04-24 G. Prior

The SNO+ experiment, currently undergoing commissioning, will be a large scale liquid scintillator detector capable of studying a variety of physics topics, with the highest priority being a sensitive search for neutrinoless double beta…

Instrumentation and Detectors · Physics 2014-05-15 Steven Biller

The SNO+ experiment, located in SNOLAB, 2 kilometers underground in the Creighton mine, near Sudbury, Canada, is a large scale neutrino detector whose main purpose is to search for neutrinoless double-beta decay and thus probe the Majorana…

Instrumentation and Detectors · Physics 2018-09-18 Vincent Fischer

We investigate the flux and the event rate of the supernova relic neutrino background (SRN) at the SuperKamiokande detector for various neutrino oscillation models with parameters inferred from recent experimental results. A realistic model…

Astrophysics · Physics 2009-11-07 S. Ando , K. Sato , T. Totani

We investigate the possibility of detecting solar electron antineutrinos with the KamLAND experiment. These electron antineutrinos are predicted by spin-flavor oscillations at a significant rate even if this mechanism is not the leading…

High Energy Physics - Phenomenology · Physics 2014-11-17 E. Torrente-Lujan