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Related papers: Standard Neutrino Spectrum from B-8 Decay

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Knowledge of the energy spectrum of $^8$B neutrinos is an important ingredient for interpreting experiments that detect energetic neutrinos from the Sun. The neutrino spectrum deviates from the allowed approximation because of the broad…

Nuclear Experiment · Physics 2013-05-29 W. T. Winter , S. J. Freedman , K. E. Rehm , J. P. Schiffer

The standard solar model (SSM) yield a $^8$B solar neutrino flux which is consistent within the theoretical and experimental uncertainties with that observed at Super-Kamiokande. The combined results from the Super- Kamiokande and the…

Astrophysics · Physics 2011-04-15 Arnon Dar

If the published event rates of the chlorine and Kamiokande solar neutrino experiments are correct, then the energy spectrum of neutrinos produced by the decay of $^8$B in the sun must be different from the energy spectrum determined from…

High Energy Physics - Phenomenology · Physics 2009-10-22 John N. Bahcall

The beta-delayed alpha spectrum from the decay of 8B has been measured with a setup that minimized systematic uncertainties that affected previous measurements. Consequently the deduced neutrino spectrum presents much smaller uncertainties…

Nuclear Experiment · Physics 2009-10-31 C. E. Ortiz , A. Garcia , R. A. Waltz , M. Bhattacharya , A. K. Komives

The next generation of solar neutrino detectors will provide a precision measure of the $^8$B electron-neutrino spectrum in the energy range from 1-15 MeV. Although the neutrino spectrum emitted by $^8$B $\beta$-decay reactions in the Sun's…

High Energy Physics - Phenomenology · Physics 2019-01-23 Ilídio Lopes , Joseph Silk

We identify and quantify systematic effects not accounted for in two previous measurements of the alpha-alpha relative-energy distribution in the beta decay of 8B, which can explain the apparent disagreement with respect to two newer…

Nuclear Experiment · Physics 2014-08-06 Oliver S. Kirsebom , Hans O. U. Fynbo , Riccardo Raabe , Karsten Riisager , Thomas Roger

The predictions of an improved standard solar model are compared with the observations of the four solar neutrino experiments. The improved model includes premain sequence evolution, element diffusion, partial ionization effects, and all…

Astrophysics · Physics 2015-06-24 Arnon Dar

The energy spectrum of recoil electrons from solar neutrino scattering, as observed by Superkamiokande, is deformed with respect to that expected from SSM calculations. We considered \nu-e scattering from neutrinos produced by the…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. L. Villante

A significant decay branch of 8B to the ground state of 8Be would extend the solar neutrino spectrum to higher energies than anticipated in the standard solar models. These high-energy neutrinos would affect current neutrino oscillation…

Nuclear Experiment · Physics 2008-11-26 M. K. Bacrania , N. M. Boyd , R. G. H. Robertson , D. W. Storm

The sensitivity of the Sudbury Neutrino Observatory (SNO) to measure the shape of the recoil electron spectrum in the charged-current reaction of $^{8}$B solar neutrinos interacting with deuterium can be improved if the results of a…

Nuclear Theory · Physics 2008-11-26 G. Jonkmans , I. S. Towner , B. Sur

Results are reported from the complete salt phase of the Sudbury Neutrino Observatory experiment in which NaCl was dissolved in the D$_2$O target. The addition of salt enhanced the signal from neutron capture, as compared to the pure D$_2$O…

Nuclear Experiment · Physics 2012-08-27 SNO Collaboration

We report a 3.3 $\sigma$ measurement of coherent elastic neutrino-nucleus scattering from solar $^8$B neutrinos using a 6.77 t$\times$yr exposure from the XENONnT experiment, inferring a solar $^8$B neutrino flux of $(5_{-2}^{+3})\times…

High Energy Physics - Experiment · Physics 2026-04-08 E. Aprile , J. Aalbers , K. Abe , M. M. Abu Rmeileh , M. Adrover , S. Ahmed Maouloud , L. Althueser , B. Andrieu , E. Angelino , D. Antón Martin , S. R. Armbruster , F. Arneodo , L. Baudis , M. Bazyk , V. Beligotti , L. Bellagamba , R. Biondi , A. Bismark , K. Boese , R. M. Braun , G. Bruni , R. Budnik , C. Cai , C. Capelli , J. M. R. Cardoso , A. P. Cimental Chávez , 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 , K. Eitel , S. el Morabit , R. Elleboro , A. Elykov , A. D. Ferella , C. Ferrari , H. Fischer , T. Flehmke , M. Flierman , R. Frankel , D. Fuchs , W. Fulgione , C. Fuselli , F. Gao , R. Giacomobono , F. Girard , R. Glade-Beucke , L. Grandi , J. Grigat , H. Guan , M. Guida , P. Gyorgy , R. Hammann , C. Hils , L. Hoetzsch , N. F. Hood , M. Iacovacci , Y. Itow , J. Jakob , F. Joerg , Y. Kaminaga , M. Kara , S. Kazama , P. Kharbanda , M. Kobayashi , D. Koke , K. Kooshkjalali , A. Kopec , E Kozlova , H. Landsman , R. F. Lang , L. Levinson , A. Li , H. Li , I. Li , S. Li , S. Liang , Z. Liang , Y. -T. Lin , S. Lindemann , M. Lindner , K. Liu , M. Liu , F. Lombardi , J. A. M. Lopes , G. M. Lucchetti , T. Luce , Y. Ma , C. Macolino , G. C. Madduri , J. Mahlstedt , F. Marignetti , T. Marrodán Undagoitia , K. Martens , J. Masbou , S. Mastroianni , V. Mazza , J. Merz , M. Messina , A. Michel , K. Miuchi , R. Miyata , A. Molinario , S. Moriyama , M. Murra , J. Müller , K. Ni , C. T. Oba Ishikawa , U. Oberlack , K. Otsuzuki , S. Ouahada , B. Paetsch , Y. Pan , Q. Pellegrini , R. Peres , J. Pienaar , M. Pierre , G. Plante , T. R. Pollmann , F. Pompa , A. Prajapati , L. Principe , J. Qin , D. Ramírez García , A. Ravindran , A. Razeto , R. Singh , L. Sanchez , J. M. F. dos Santos , I. Sarnoff , G. Sartorelli , M. T. Schiller , P. Schulte , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , F. N. Semler , P. Shagin , S. Shi , H. Simgen , Z. Song , A. Stevens , C. Szyszka , A. Takeda , Y. Takeuchi , P. -L. Tan , D. Thers , G. Trinchero , C. D. Tunnell , K. Valerius , S. Vecchi , S. Vetter , G. Volta , B. von Krosigk , C. Weinheimer , D. Wenz , C. Wittweg , V. H. S. Wu , Y. Xing , D. Xu , Z. Xu , M. Yamashita , J. Yang , L. Yang , J. Ye , M. Yoshida , L. Yuan , G. Zavattini , Y. Zhao , M. Zhong , T. Zhu

The Standard Solar Model (BP04) predicts a total 8B neutrino flux that is 17.2% larger than measured in the salt phase of the SNO detector (and if it were significant it will indicate oscillation to sterile neutrinos). Hence it is important…

Nuclear Experiment · Physics 2008-11-26 Moshe Gai

A search for inverse beta decay electron antineutrinos has been carried out using the 825 days sample of solar data obtained at SK. The absence of a significant signal, that is, contributions to the total SK background and their angular…

High Energy Physics - Phenomenology · Physics 2009-10-31 E. Torrente-Lujan

We report the measurement of electron neutrino elastic scattering from 8B solar neutrinos with 3 MeV energy threshold by the Borexino detector in Gran Sasso (Italy). The rate of solar neutrino-induced electron scattering events above this…

Astrophysics · Physics 2015-03-13 The Borexino Collaboration

The $^8$B solar neutrino flux predicted by the standard solar model (SSM) is consistent within the theoretical and experimental uncertainties with that observed at Kamiokande. The Gallium and Chlorine solar neutrino experiments, however,…

Astrophysics · Physics 2007-05-23 Arnon Dar

By combining the results of SNO and Super-Kamiokande one can derive - in the absence of sterile neutrinos - the total neutrino flux produced from $^8$B decay in the Sun. We use this information to check the accuracy of several input…

Astrophysics · Physics 2009-11-07 G. Fiorentini , B. Ricci

Results are reported from a joint analysis of Phase I and Phase II data from the Sudbury Neutrino Observatory. The effective electron kinetic energy threshold used is T_eff=3.5 MeV, the lowest analysis threshold yet achieved with water…

Nuclear Experiment · Physics 2015-03-13 The SNO Collaboration

In recent years, interest in experimental studies of $\beta$-decay electron spectra -- often referred to as $\beta$ spectra -- has been growing. This is particularly true for $\beta$ transitions where the electron spectra are sensitive to…

The SNO+ detector operated initially as a water Cherenkov detector. The implementation of a sealed covergas system midway through water data taking resulted in a significant reduction in the activity of $^{222}$Rn daughters in the detector…

High Energy Physics - Experiment · Physics 2024-12-24 SNO+ Collaboration , : , A. Allega , M. R. Anderson , S. Andringa , M. Askins , D. M. Asner , D. J. Auty , A. Bacon , F. Barão , N. Barros , R. Bayes , E. W. Beier , A. Bialek , S. D. Biller , E. Blucher , E. Caden , E. J. Callaghan , M. Chen , S. Cheng , B. Cleveland , D. Cookman , J. Corning , M. A. Cox , R. Dehghani , J. Deloye , M. M. Depatie , F. Di Lodovico , C. Dima , J. Dittmer , K. H. Dixon , M. S. Esmaeilian , E. Falk , N. Fatemighomi , R. Ford , A. Gaur , O. I. González-Reina , D. Gooding , C. Grant , J. Grove , S. Hall , A. L. Hallin , D. Hallman , W. J. Heintzelman , R. L. Helmer , C. Hewitt , B. Hreljac , J. Hu , P. Huang , R. Hunt-Stokes , S. M. A. Hussain , A. S. Inácio , C. J. Jillings , S. Kaluzienski , T. Kaptanoglu , J. Kladnik , J. R. Klein , L. L. Kormos , B. Krar , C. Kraus , C. B. Krauss , T. Kroupová , C. Lake , L. Lebanowski , C. Lefebvre , V. Lozza , M. Luo , A. Maio , S. Manecki , J. Maneira , R. D. Martin , N. McCauley , A. B. McDonald , G. Milton , D. Morris , M. Mubasher , S. Naugle , L. J. Nolan , H. M. O'Keeffe , G. D. Orebi Gann , J. Page , K. Paleshi , W. Parker , J. Paton , S. J. M. Peeters , L. Pickard , B. Quenallata , P. Ravi , A. Reichold , S. Riccetto , J. Rose , R. Rosero , I. Semenec , J. Simms , P. Skensved , M. Smiley , R. Svoboda , B. Tam , J. Tseng , E. Vázquez-Jáuregui , C. J. Virtue , M. Ward , J. R. Wilson , J. D. Wilson , A. Wright , S. Yang , M. Yeh , Z. Ye , S. Yu , Y. Zhang , K. Zuber , A. Zummo
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