Physics Letters B 795 (2019) 542–547
Contents lists available at ScienceDirect
Physics Letters B
www.elsevier.com/locate/physletb
The gallium anomaly revisited
J. Kostensalo
a,∗
, J. Suhonen
a
, C. Giunti
b
, P.C. Srivastava
c
a
University of Jyvaskyla, Department of Physics, P.O. Box 35, FI-40014, Finland
b
INFN, Sezione di Torino, Via P. Giuria 1, I-10125 Torino, Italy
c
Department of Physics, Indian Institute of Technology, Roorkee 247667, India
a r t i c l e i n f o a b s t r a c t
Article history:
Received
26 June 2019
Accepted
27 June 2019
Available
online 2 July 2019
Editor: W.
Haxton
Keywords:
Gallium
anomaly
Charged-current
cross-sections
Nuclear
shell model
Neutrino-nucleus
interactions
The gallium anomaly, i.e. the missing electron-neutrino flux from
37
Ar and
51
Cr electron-capture decays
as measured by the GALLEX and SAGE solar-neutrino detectors, has been among us already for about
two decades. We present here a new estimate of the significance of this anomaly based on cross-section
calculations using nuclear shell-model wave functions obtained by exploiting recently developed two-
nucleon
interactions. The gallium anomaly of the GALLEX and SAGE experiments is found to be smaller
than that obtained in previous evaluations, decreasing the significance from 3.0σ to 2.3σ . This result is
compatible with the recent indication in favor of short-baseline
¯
ν
e
disappearance due to small active-
sterile
neutrino mixing obtained from the combined analysis of the data of the NEOS and DANSS reactor
experiments.
© 2019 Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP
3
.
1. Introduction
Gallium-based solar-neutrino experiments, GALLEX [1–3] and
SAGE [4], were designed to detect pp neutrinos from the sun.
These two experiments are unique in having been tested for their
detection efficiency by
37
Ar and
51
Cr radioactive sources. These
sources emit discrete-energy electron neutrinos (E
ν
< 1MeV)
based on their decay via nuclear electron capture (EC). Detection of
these neutrinos is achieved through the charged-current neutrino-
nucleus
scattering reaction
ν
e
+
71
Ga(3/2
−
)
g.s.
→
71
Ge( J
π
) +e
−
(1)
to the lowest four (flux from the
51
Cr source) or five (flux from the
37
Ar source) nuclear states in
71
Ge. In this article we discuss also
the analogous reaction
ν
e
+
69
Ga(3/2
−
)
g.s.
→
69
Ge( J
π
) +e
−
(2)
in order to test our calculated shell-model wave functions more
comprehensively.
The
scattering of
37
Ar and
51
Cr neutrinos off
71
Ga leads mainly
to the ground state and the excited states at 175 keV and 500
*
Corresponding author.
E-mail
address: joel.j.kostensalo@student.jyu.fi (J. Kostensalo).
keV in
71
Ge. The scattering cross sections for the mentioned three
low-lying states can be estimated by using the data from charge-
exchange
reactions [5]or by using a microscopic nuclear model,
like the nuclear shell model [6]. In both cases it has been found
that the estimated cross sections are larger than the ones mea-
sured
by the GALLEX [1–3]and SAGE [4] experiments. The mea-
sured
neutrino capture rates (cross sections) are 0.87 ± 0.05 of
the rates based on the cross-section estimates by Bahcall [6]. The
related model calculations and analyses based on them have been
discussed in [7–9]. It should be noted that the response to the
ground state is known from the electron-capture ft value of
71
Ge.
The discrepancy between the measured and theoretical capture
rates constitutes the so-called “gallium anomaly”.
One
of the explanations to the gallium anomaly is associated
with the oscillation of the electron neutrinos to a sterile neutrino
in eV mass scale [7,9]. The same scheme could also explain the
so-called “reactor-antineutrino anomaly” [10–12], discussed, e.g. in
[9]. Searches for the sterile neutrinos are under progress in sev-
eral
laboratories. However, it should be remarked here that there
is no accepted sterile neutrino model to explain the experimen-
tal
anomalies consistently, and also alternative solutions to the
reactor-antineutrino anomaly have been proposed, like the proper
inclusion of first-forbidden β-decay branches in the construction
of the cumulative antineutrino spectra [13].
https://doi.org/10.1016/j.physletb.2019.06.057
0370-2693/
© 2019 Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP
3
.