Hunting sub-GeV dark matter with the NOνA near detector
Patrick deNiverville
Center for Theoretical Physics of the Universe, IBS, Daej eon 34126, Korea
Claudia Frugiuele
Department of Particle Physics and Astrophysics, Weizmann Institute of Science, Rehovot 76100, Israel
(Received 7 August 2018; published 6 March 2019)
We study the sensitivity of the NOνA near detector to MeV-GeV dark matter while operating
symbiotically with the neutrino program. We find that NOν A could explore a large new region of parameter
space over the next few years for dark matter masses below 100 MeV, reaching the thermal target for a
scalar dark matter particle for some masses. This result represents a significant improvement over existing
probes such as BABAR, E137, MiniBooNE, and LSND.
DOI: 10.1103/PhysRevD.99.051701
I. INTRODUCTION
There are many compelling dark matter (DM) candidates
with a correspondingly wide range of possible masses and
couplings to the visible sector. Probing this vast parameter
space requires a correspondingly broad experimental pro-
gram, and neutrino fixed target facilities can play a role in
this quest by searching for signatures of DM scattering with
electrons and/or nuclei in their (near) detectors [1–10].
Their main advantage lies in the high luminosity available,
frequently boasting 10
20
–10
21
protons on target (POT) per
year, which allows for the production of a sizeable
relativistic DM beam. Moreover, this setup offers the
possibility of probing light DM/quark couplings, comple-
mentary to direct detection experiments sensitive to elec-
tron/DM interactions [11,12].
However, the neutrino background presents a significant
challenge when searching for nucleon-DM scattering
[2,4,5,7–9]. More promising in this regard is electron-
DM scattering, where the neutrino related backgrounds are
much smaller. Some of the strongest constraints on the DM
parameter space have been placed by recasting existing
neutrino-electron scattering data from the LSND experi-
ment [13,14] and we aim to investigate whether present
neutrino facilities could improve on LSND’s sensitivity. In
particular, we study the reach of the NOνA near detector to
DM-electron scattering. By reinterpreting an existing
analysis on ν − e elastic scattering we find sensitivity to
a large region of the DM parameter space still uncon-
strained by present experimental probes such as LSND
[13,14], E137 [15], MiniBooNE [16,17],NA64[18],
BABAR [19] and CRESST-II [20].
The paper is organized as follow: in Sec. II we define our
benchmark model. Section III summarizes the main aspects
of DM searches at neutrino facilities. In Sec. IV, we present
the sensitivity of NOVνA of electron-DM elastic scattering
by recasting of current analysis performed by the collab-
orations. Finally, we present a summary in Sec. V.
II. VECTOR PORTAL
Our benchmark model consists of a dark photon (DP)
[21] A
0
μ
, the gauge boson of a new dark gauge group Uð1 Þ
D
kinetically mixed with the photon, and a scalar χ charged
under Uð1Þ
D
that serves as a DM candidate:
L
DM
¼ L
A
0
þ L
χ
ð1Þ
where:
L
A
0
¼ −
1
4
F
0
μν
F
0μν
þ
m
2
A
0
2
A
0μ
A
0
μ
−
1
2
ϵF
0
μν
F
μν
; ð2Þ
where ϵ is the DP-photon kinetic mixing, while:
L
χ
¼
ig
D
2
A
0μ
J
χ
μ
þ
1
2
∂
μ
χ
†
∂
μ
χ − m
2
χ
χ
†
χ; ð3Þ
where J
χ
μ
¼½ð∂
μ
χ
†
Þχ − χ
†
∂
μ
χ and g
D
is the Uð1Þ
D
gauge
coupling. The region of the parameter space reachable by
neutrino facilities is m
A
0
> 2m
χ
and g
D
≫ ϵe which
implies that the DP almost always decays into a χχ
†
pair.
For much of the parameter space studied, the strongest
experimental constraints for m
χ
> 60 MeV come from a
monophoton search performed by BABAR [19] that exclu-
des the existence of a DP with ϵ > 10
−3
and m
A
0
< 8 GeV
decaying into χ
¯
χ. For large values of α
D
, CRESST-II
places strong constraints on m
χ
> 500 MeV. The NA64
Published by the American Physical Society unde r the terms of
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the author(s) and the published article’s title, journal citation,
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3
.
PHYSICAL REVIEW D 99, 051701(R) (2019)
Rapid Communications
2470-0010=2019=99(5)=051701(6) 051701-1 Published by the American Physical Society