Measurement of the Total Active<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">B</mml:mi><mml:mprescripts/><mml:none/><mml:mn>8</mml:mn></mml:mmultiscripts></mml:math>Solar Neutrino Flux at the Sudbury Neutrino Observatory with Enhanced Neutral Current Sensitivity

S. N. Ahmed(Queen's University), A. E. Anthony(The University of Texas at Austin), E. W. Beier(University of Pennsylvania), A. Bellerive(Carleton University), S. D. Biller(University of Oxford), J. Boger(Brookhaven National Laboratory), M. G. Boulay(Los Alamos National Laboratory), M. G. Bowler(University of Oxford), T. J. Bowles(Los Alamos National Laboratory), S. J. Brice(Los Alamos National Laboratory), T. V. Bullard(University of Washington), Y. D. Chan(Lawrence Berkeley National Laboratory), M. Chen(Queen's University), X. Chen(Lawrence Berkeley National Laboratory), B. T. Cleveland(University of Oxford), G. A. Cox(University of Washington), X. Dai(University of Oxford), F. Dalnoki‐Veress(Carleton University), P. J. Doe(University of Washington), R.S. Dosanjh(Carleton University), G. Doucas(University of Oxford), M. R. Dragowsky(Los Alamos National Laboratory), C. A. Duba(University of Washington), F. A. Duncan(Queen's University), M. Dunford(University of Pennsylvania), J. Dunmore(University of Oxford), E. D. Earle(Queen's University), S. R. Elliott(Los Alamos National Laboratory), H. C. Evans(Queen's University), G. T. Ewan(Queen's University), J. Farine(Carleton University), H. Fergani(University of Oxford), F. Fleurot(Laurentian University), J. A. Formaggio(University of Washington), M. M. Fowler(Los Alamos National Laboratory), K. C. Frame(University of Oxford), B. G. Fulsom(Queen's University), N. Gagnon(University of Washington), K. Graham(Queen's University), D. R. Grant(Carleton University), R. L. Hahn(Brookhaven National Laboratory), James C. Hall(The University of Texas at Austin), A. L. Hallin(Queen's University), E. D. Hallman(Laurentian University), A. S. Hamer(Los Alamos National Laboratory), W. B. Handler(Queen's University), C. K. Hargrove(Carleton University), P. J. Harvey(Queen's University), R. Hazama(University of Washington), K. M. Heeger(Lawrence Berkeley National Laboratory), W. J. Heintzelman(University of Pennsylvania), J. Heise(Los Alamos National Laboratory), R. L. Helmer(TRIUMF), R.J. Hemingway(Carleton University), A. Hime(Los Alamos National Laboratory), M. A. Howe(University of Washington), P. Jagam(University of Guelph), N.A. Jelley(University of Oxford), J. R. Klein(University of Pennsylvania), M. Kos(Queen's University), A. V. Krumins(Queen's University), T. Kutter(University of British Columbia), Christopher C. M. Kyba(University of Pennsylvania), H. Labranche(University of Guelph), R. Lange(Brookhaven National Laboratory), J. Law(University of Guelph), I. Lawson(University of Guelph), K. T. Lesko(Lawrence Berkeley National Laboratory), J. R. Leslie(Queen's University), I. Levine(Carleton University), S. Luoma(Laurentian University), R. MacLellan(Queen's University), Steve Majerus(University of Oxford), H.‐B. Mak(Queen's University), J. Maneira(Queen's University), A. D. Marino(Lawrence Berkeley National Laboratory), N. McCauley(University of Pennsylvania), A. B. McDonald(Queen's University), S. McGee(University of Washington), G. McGregor(University of Oxford), C. Mifflin(Carleton University), K. K. S. Miknaitis(University of Washington), Guthrie Miller(Los Alamos National Laboratory), B. A. Moffat(Queen's University), C. W. Nally(University of British Columbia), B. G. Nickel(University of Guelph), A. J. Noble(Queen's University), E. B. Norman(Lawrence Berkeley National Laboratory), N. S. Oblath(University of Washington), C. Okada(Lawrence Berkeley National Laboratory), R. W. Ollerhead(University of Guelph), J. L. Orrell(University of Washington), S. M. Oser(University of British Columbia), C. Ouellet(Queen's University), S. J. M. Peeters(University of Oxford), A. W. P. Poon(Lawrence Berkeley National Laboratory), B.C. Robertson(Queen's University), R. G. H. Robertson(University of Washington), E. Rollin(Carleton University), S. S. E. Rosendahl(Lawrence Berkeley National Laboratory), Vadim Rusu(University of Pennsylvania), M. H. Schwendener(Laurentian University), O. Simard(Carleton University), J. J. Simpson(University of Guelph), C. J. Sims(University of Oxford), D. Sinclair(TRIUMF), P. Skensved(Queen's University), M. W. E. Smith(University of Washington), N. Starinsky(Carleton University), R. G. Stokstad(Lawrence Berkeley National Laboratory), L. C. Stonehill(University of Washington), R. Tafirout(Laurentian University), Y. Takeuchi(Queen's University), G. Tešić(Carleton University), M. Thomson(Queen's University), M. Thorman(University of Oxford), R. Van Berg(University of Pennsylvania), R. G. Van de Water(Los Alamos National Laboratory), C. J. Virtue(Laurentian University), B. L. Wall(University of Washington), D. Waller(Carleton University), Chris Waltham(University of British Columbia), H. Wan Chan Tseung(University of Oxford), D. L. Wark(Rutherford Appleton Laboratory), N. West(University of Oxford), J.B. Wilhelmy(Los Alamos National Laboratory), J. F. Wilkerson(University of Washington), J. R. Wilson(University of Oxford), J.M. Wouters(Los Alamos National Laboratory), M. Yeh(Brookhaven National Laboratory), Κ. Zuber(University of Oxford)
Physical Review Letters
May 3, 2004
Cited by 773Open Access
Full Text

Abstract

The Sudbury Neutrino Observatory has precisely determined the total active (${\ensuremath{\nu}}_{x}$) $^{8}\mathrm{B}$ solar neutrino flux without assumptions about the energy dependence of the ${\ensuremath{\nu}}_{e}$ survival probability. The measurements were made with dissolved NaCl in heavy water to enhance the sensitivity and signature for neutral-current interactions. The flux is found to be $5.21\ifmmode\pm\else\textpm\fi{}0.27\mathrm{(}\mathrm{stat}\mathrm{)}\ifmmode\pm\else\textpm\fi{}0.38\mathrm{(}\mathrm{syst}\mathrm{)}\ifmmode\times\else\texttimes\fi{}{10}^{6}\text{ }{\mathrm{cm}}^{\ensuremath{-}2}\text{ }\text{ }{\mathrm{s}}^{\ensuremath{-}1}$, in agreement with previous measurements and standard solar models. A global analysis of these and other solar and reactor neutrino results yields $\ensuremath{\Delta}{m}^{2}={7.1}_{\ensuremath{-}0.6}^{+1.2}\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}\text{ }{\mathrm{eV}}^{2}$ and $\ensuremath{\theta}={32.5}_{\ensuremath{-}2.3}^{+2.4}$ degrees. Maximal mixing is rejected at the equivalent of 5.4 standard deviations.


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