Published 1994 | Version v1
Report Open

Boron neutrino flux and the MSW solution of the solar neutrino problem

  • 1. North Carolina Univ., Chapel Hill, NC (United States)
  • 2. International Centre for Theoretical Physics, Trieste (Italy)
  • 3. Washington Univ., Seattle, WA (United States). Inst. for Nuclear Theory

Description

There are large uncertainties in the predictions of the boron neutrino flux from the Sun which cannot be considered as being of purely statistical origin. We treat the magnitude of this flux, ΦB, as a parameter to be found from experiment. The properties of the, MSW solution to the solar neutrino problem for different values of ΦB are studied. Present, data give the bounds: 0.38 < ΦB/ΦBO < 3.1 (2σ), where ΦBO ≡ 5.7 · 106 cm-2s-1 is the flux in the reference SSM. The variations of the flux in this interval enlarge the allowed region of mixing angles: sin2 2θ = 0.2 divided-by 2 · 10-4 divided-by 2 · 10-2 (small mixing solutions) and sin2 2θ = 0.2 divided-by 0.85 (large mixing solution). If the value of the original boron neutrino flux is about that measured by Kamiokande, a consistent description of the data is achieved for sin2 2θ ∼ (0.8 divided-by 2) · 10-3 (''very small mixing solution''). The solution is characterized by a strong suppression of the beryllium neutrino line, a weak distortion of the high energy part of the baron neutrino spectrum and a value of the double ratio (CC/NC)exp/(CC/NC)SSM at E > 5 MeV close to 1. We comment on the possibility to measure the neutrino parameters and the original boron neutrino flux in future experiments

Availability note (English)

MF available from INIS under the Report Number; Also available from OSTI as DE95001861; NTIS; US Govt. Printing Office Dep.

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Additional details

Publishing Information

Imprint Pagination
19 p.
Report number
DOE/ER/40561--137

Optional Information

Contract/Grant/Project number
Contract FG06-90ER40561; FG05-85ER40219
Funding organization
USDOE, Washington, DC (United States).
Secondary number(s)
FNAL/Pub--94/179-T.