|
Only neutrinos,
with their extremely small interaction cross sections,
can enable us to see into the interior of a star, and thus verify directly the hypothesis of nuclear energy generation in stars. |
| John N. Bahcall (1964) |
Solar Neutrino Experiments
Bahcall et al.
Standard Solar Models:
BU88,
BP92,
BP95,
BP98,
BP00,
BP04,
BS05.
Software and Data by J.
Bahcall.
New (June 2002):
7Be line shape data,
from
Phys.
Rev.
D 49 (1994) 3923.
Has some effect in the BOREXino predictions for some part of the space of parameters (Carlos Peña Garay).
The damping of oscillations due to the
7Be line shape is more important than averaging over the radial distribution of neutrino production in the Sun (John Bahcall).
See:
Fogli,
Lisi,
Montanino,
Palazzo,
PRD 62,
113004 (2000),
hep-ph/0005261,
Sec.
VI and Fig.
5,
and
Lisi,
Marrone,
Montanino,
Palazzo,
Petcov,
PRD 63,
093002 (2001),
hep-ph/0011306,
Fig.
8 and related comments.
Super-Kamiokande-I Solar Neutrino Data
Tables and Figures of Neutrino (Anti-Neutrino) Deuteron Reactions Cross Sections
Living Reviews in Solar Physics
Solar Physics
(NASA's Marshall Space Flight Center)
Solar Physics Glossary
The Solar and Heliospheric Observatory (SOHO)
APS Neutrino Study: Solar and Atmospheric Neutrino Experiments Working Group
NASA Astronomy Picture of the Day (5 June 1998): Neutrinos in the Sun
1 - Books
2 - Reviews - Experiment
3 - Reviews - Experiment - Conference Proceedings
4 - Reviews - Experiment - Slides
5 - Reviews - History
6 - Reviews - Astrophysics
7 - Reviews - Astrophysics - Conference Proceedings
8 - Reviews - Phenomenology
9 - Reviews - Phenomenology - Conference Proceedings
10 - Experiment
11 - Experiment - Conference Proceedings
12 - Experiment - Slides
13 - Experiment - Neutrino Oscillations
14 - Experiment - Neutrino Oscillations - Conference Proceedings
15 - Experiment - Neutrino Oscillations - Slides
16 - Experiment - Astrophysical Cross Sections
17 - Experiment - Background
18 - Experiment - Astrophysics
19 - Standard Solar Model
20 - Standard Solar Model - Conference Proceedings
21 - Non-Standard Solar Models
22 - Astrophysics
23 - Astrophysics - Conference Proceedings
24 - Astrophysical Cross Sections
25 - Astrophysical Cross Sections - Conference Proceedings
26 - Detection Cross Sections
27 - Detection Cross Sections - Conference Proceedings
28 - Detector
29 - Phenomenology
30 - Phenomenology - Conference Proceedings
31 - Phenomenology - Models
32 - Phenomenology - Slides
33 - Phenomenology - Background
34 - Phenomenology - Gallium Anomaly
35 - Phenomenology - Gallium Anomaly - Conference Proceedings
36 - Theory
37 - Future Projects
38 - Future Projects - Conference Proceedings
39 - Education
40 - History
41 - History - Conference Proceedings
C.L.
allowed contours for
oscillations obtained by different atmospheric neutrino experiments.
The
figure
in slide n.24 shows the
C.L.
allowed contour for
oscillations obtained by Super-Kamiokande.
[M.L.].
and Total
B Solar Neutrino Fluxes with the Sudbury Neutrino Observatory Phase-III Data Set,
B. Aharmim et al.
(SNO),
arXiv:1107.2901, 2011.
solar neutrino rate in Borexino and MSW oscillation parameters,
G. Bellini et al.
(Borexino),
Phys. Lett. B707 (2012) 22-26,
arXiv:1104.2150.
solar neutrino interaction rate in Borexino,
G. Bellini et al.
(Borexino),
(2011),
arXiv:1104.1816.
Solar Neutrino Flux at the Sudbury Neutrino Observatory,
B. Aharmim et al.
(SNO),
Astrophys. J. 710 (2010) 540-548,
arXiv:0910.2433.
neutrino flux with 246 live days of Borexino and observation of the MSW vacuum-matter transition,
G. Bellini et al.
(BOREXino),
Phys. Rev. D82 (2010) 033006,
arXiv:0808.2868.
solar neutrinos by BOREXino,
C. Arpesella et al.
(BOREXino),
Phys. Lett. B658 (2008) 101-108,
arXiv:0708.2251.
and Total
Solar Neutrino Fluxes with the Sudbury Neutrino Observatory Phase I Data Set,
B. Aharmim et al.
(SNO),
Phys. Rev. C75 (2007) 045502,
arXiv:nucl-ex/0610020.
Solar Neutrino Flux Measured by the Sudbury Neutrino Observatory,
B. Aharmim et al.
(SNO),
Phys. Rev. D72 (2005) 052010,
arXiv:hep-ex/0507079.
neutrino flux by the Earth's orbital eccentricity.
No significant sinusoidal periodicities are found with periods between 1 day and 10 years.
Solar Neutrinos from the 391-Day Salt Phase SNO Data Set,
B. Aharmim et al.
(SNO),
Phys. Rev. C72 (2005) 055502,
arXiv:nucl-ex/0502021.
from the sun at Super-Kamiokande-I,
Y. Gando et al.
(Super-Kamiokande),
Phys. Rev. Lett. 90 (2003) 171302,
arXiv:hep-ex/0212067.
spectrum the upper limit to the solar
flux is
of the SSM
flux prediction for total energy = 8 Mev - 20 MeV.
Interactions Produced by
B Solar Neutrinos at the Sudbury Neutrino Observatory,
Ahmad, Q. R. et al.
(SNO),
Phys. Rev. Lett. 87 (2001) 071301,
arXiv:nucl-ex/0106015.
and
neutrino measurements from 1258 days of Super-Kamiokande data,
Fukuda, S. et al.
(Super-Kamiokande),
Phys. Rev. Lett. 86 (2001) 5651-5655,
arXiv:hep-ex/0103032.
.
disappearance,
Gratta, G.
(Kamland), 2002.
SLAC Colloquium,
December 2002.
http://hep.stanford.edu/neutrino/KamLAND/TalksAndPublications/KamLAND_FirstResults_SLAC_Colloq.pdf.
and
.
's from the Sun and Other Sources at KamLAND,
K. Eguchi et al.
(KamLAND),
Phys. Rev. Lett. 92 (2004) 071301,
arXiv:hep-ex/0310047.
's in the energy range
.
No candidates were found for an expected background of
events.
This result can be used to obtain a limit on
fluxes of any origin.
Assuming that all
flux has its origin in the Sun and has the characteristic
solar
energy spectrum,
we obtain an upper limit of
(90% C.L.) on the
flux.
We interpret this limit,
corresponding to
of the Standard Solar Model
flux,
in the framework of spin-flavor precession and neutrino decay models.
disappearance,
Gratta, G.
(Kamland), 2002.
SLAC Colloquium,
December 2002.
http://hep.stanford.edu/neutrino/KamLAND/TalksAndPublications/KamLAND_FirstResults_SLAC_Colloq.pdf.
S-factor,
Junghans, A. R. et al.,
Phys. Rev. C68 (2003) 065803,
arXiv:nucl-ex/0308003.
,
Motobayashi, T.,
Nucl. Phys. A693 (2001) 258-268.
cross section,
Hammache, F. et al.,
Nucl. Phys. A688 (2001) 273-276.
reaction with radioactive beams and the
solar neutrino flux,
Gai, Moshe,
Prog. Part. Nucl. Phys. 46 (2001) 89-96,
arXiv:nucl-ex/0010014.
theoretical uncertainties.
B neutrino flux calculated with the older and larger heavy element abundances (or with the newer and lower heavy element abundances) to the total neutrino flux measured by the Sudbury Neutrino Observatory is 1.09 (0.87) with a 9% experimental uncertainty and a 16% theoretical uncertainty,
errors.
and
neutrinos agree with the experimentally-determined fluxes (including oscillations):
,
and
,
experimental and theoretical uncertainties,
respectively.
neutrino flux is the only significant change in the best-estimate fluxes.
reaction,
solar neutrinos and the age of the globular clusters,
S. Degl'Innocenti, G. Fiorentini, B. Ricci, F.L. Villante,
Phys. Lett. B590 (2004) 13,
arXiv:astro-ph/0312559.
,
Motobayashi, T.,
Nucl. Phys. A693 (2001) 258-268.
cross section,
Hammache, F. et al.,
Nucl. Phys. A688 (2001) 273-276.
reaction with radioactive beams and the
solar neutrino flux,
Gai, Moshe,
Prog. Part. Nucl. Phys. 46 (2001) 89-96,
arXiv:nucl-ex/0010014.
reaction and the solar neutrino problem,
Marcucci, L. E.,
Nucl. Phys. A689 (2001) 280-289,
arXiv:nucl-th/0009066.
asymp.
normalization coefficients (nucl.
vertex constants) and their application for extrapolation of the
astroph.
S-factors to the solar energy region,
Igamov, S. B., Tursunmakhatov, K. I., Yarmukhamedov, R.,
arXiv:0905.2026, 2009.
S-factor from ab initio no-core shell model wave functions,
P. Navratil, C.A. Bertulani, E. Caurier,
Phys. Rev. C73 (2006) 065801,
arXiv:nucl-th/0601019.
and
and the astrophysical
factor,
G. Tabacaru et al.,
Phys. Rev. C73 (2006) 025808,
arXiv:nucl-ex/0508029.
factor from a measurement of
reaction at
,
J.J. Das et al.,
arXiv:nucl-ex/0409017, 2004.
neutrino spectrum,
Winter, W. T., Freedman, S. J., Rehm, K. E., Schiffer, J. P.,
Phys. Rev. C73 (2006) 025503,
arXiv:nucl-ex/0406019.
from published data,
R. H. Cyburt, B. Davids, B. K. Jennings,
Phys. Rev. C70 (2004) 045801,
arXiv:nucl-th/0406011.
and the astrophysical
factor for
,
B. Davids, S. Typel,
Phys. Rev. C68 (2003) 045802,
arXiv:nucl-th/0304054.
of
(95% confidence level).
reaction rate would no longer represent the dominant uncertainty in the theoretical prediction of the high-energy solar neutrino flux.
(see [41-1]),
taken from [6-8].
B Decay,
Bahcall, J. N. et al.,
Phys. Rev. C54 (1996) 411-422,
arXiv:nucl-th/9601044.
,
W.H. Lippincott et al.,
Phys. Rev. C81 (2010) 045803,
arXiv:0911.5453.
independent of reactor antineutrino fluxes,
Antonio Palazzo,
arXiv:1201.4280, 2012.
in Different Mixing Matrix Parametrizations,
Melin Huang, S. D. Reitzner, Wei-Chun Tsai, Huitzu Tu,
arXiv:1111.3175, 2011.
from Solar and KamLAND Neutrino Data,
H.L. Ge, C. Giunti, Q.Y. Liu,
Phys. Rev. D80 (2009) 053009,
arXiv:0810.5443.
Be Neutrino Signal Variation in KamLAND,
Bhag C. Chauhan,
JHEP 0602 (2006) 035,
arXiv:hep-ph/0510415.
,
Kopylov, Anatoly,
arXiv:hep-ph/0411031, 2004.
in Solar and Reactor Neutrino Experiments,
Abhijit Bandyopadhyay, Sandhya Choubey, Srubabati Goswami, S.T. Petcov,
Phys. Rev. D72 (2005) 033013,
arXiv:hep-ph/0410283.
are either
or
.
give
in LSND.
Therefore,
this case is equivalent to neglect LSND.
obviously cannot fit the energy spectra of atmospheric neutrinos,
which have been omitted in the analysis.
solar neutrino flux is
times the flux predicted by the BP00 standard solar model;
the
Be neutrino flux is
the predicted flux;
and the
B flux is
the predicted flux.
The oscillation parameters are:
and
.
Be
scattering experiment accurate to
% can reduce the uncertainty in the experimentally determined
Be neutrino flux by a factor of four and the uncertainty in the
neutrino flux by a factor of 2.5 (to
%).
A future
experiment must be accurate to better than
% to shrink the uncertainty in
by more than 15%.
,
Abhijit Bandyopadhyay, Sandhya Choubey, Srubabati Goswami,
Phys. Rev. D67 (2003) 113011,
arXiv:hep-ph/0302243.
has been found.
(M.L.).
.
or
in the flux of solar neutrinos on Earth?,
Giunti, C.,
Phys. Rev. D65 (2002) 033006,
arXiv:hep-ph/0107310.
with rapidly oscillating
solar neutrinos,
Baltz, A. J.,
Phys. Rev. D65 (2002) 053005,
arXiv:hep-ph/0106339.
transition solution of the solar neutrino problem,
Krastev, P. I., Petcov, S. T., Qiuyu, L.,
Phys. Rev. D54 (1996) 7057-7066,
arXiv:hep-ph/9602333.