Monoenergetic Neutrinos from WIMP Annihilation in Jupiter George M. Frenchand Marc Shery High Energy Theory Group Department of Physics

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Monoenergetic Neutrinos from WIMP Annihilation in Jupiter
George M. Frenchand Marc Sher
High Energy Theory Group, Department of Physics,
William & Mary, Williamsburg, VA 23187-8795, USA
(Dated: December 14, 2022)
Abstract
Weakly interacting massive particles (WIMPs) can be captured by the Sun and annihilate in
the core, which may result in production of kaons that can decay at rest into monoenergetic 236
MeV neutrinos. Several studies of detection of these neutrinos at DUNE have been carried out.
It has been shown that if the WIMP mass is below 4 GeV, then they will evaporate prior to
annihilation, suppressing the signal. Since Jupiter has a cooler core, WIMPs with masses in the
1-4 GeV range will not evaporate and can thus annihilate into kaons which decay at rest into
monoenergetic neutrinos. We calculate the flux of these neutrinos near the surface of Jupiter and
find that it is comparable to the flux of neutrinos from the Sun at DUNE for masses above 4
GeV and substantially greater in the 1-4 GeV range. Of course, detecting these neutrinos would
require a neutrino detector near Jupiter. Obviously, it will be many decades before such a detector
can be built, but should direct detection experiments find a WIMP with a mass in the 1-4 GeV
range, it may be one of the few ways to learn about the annihilation process. A liquid hydrogen
time projection chamber might be able to get precise directional information and energy of these
neutrinos (and hydrogen is plentiful in the vicinity of Jupiter). We speculate that such a detector
could be placed on the far side of one of the tidally locked Amalthean moons; the moon itself would
provide substantial background shielding and the surface would allow easier deployment of solar
panels for power generation.
gmfrench@email.wm.edu
mtsher@wm.edu
1
arXiv:2210.04761v2 [hep-ph] 13 Dec 2022
I. INTRODUCTION
Weakly interacting massive particles (WIMPs) are one of the main candidates for dark
matter. The primary detection strategies for detection of WIMPs are production at colliders,
direct detection in underground experiments and indirect detection from WIMP annihilation.
The efficacy of each of these strategies is very dependent on the mass and interactions of
the WIMPs, and thus all three must be deployed. It has been noted [18] that WIMPs can
be gravitationally captured by the Sun, resulting in a much higher WIMP density in the
Sun, leading to annihilation into neutrinos (most other annihilation products will not be
detectable outside the Sun). Searches for high energy neutrinos from WIMP annihilation
in the Sun have been carried out [911]. It was later pointed out [12,13] that in models in
which the WIMPs annihilate into light quarks (or heavy quarks which then decay into light
quarks) there will be a large number of low-energy (sub-GeV) neutrinos produced. These
papers focused on decays of muons and pions. However, in a series of papers by Rott, In,
Kumar and Yaylali (RIKY) [1416], it was argued that the pions and kaons would come
to rest before decaying and thus would decay into monoenergetic neutrinos. Pions yield 32
MeV neutrinos and kaons yield (64% of the time) 236 MeV neutrinos. RIKY noted that
WIMPs with masses below 3-4 GeV would evaporate, but that masses in the 4 10 GeV
range would cover a region of parameter-space which could be detected at DUNE and would
not be excluded by direct detection experiments. A flux of 236 MeV neutrinos coming from
the Sun would be a smoking gun for dark matter annihilation. Recently, DUNE [17] has
analyzed this possibility and shown that spin-dependent cross-sections as low as 1038cm2
can be reached.
Detection of a monoenergetic flux of neutrinos from the Sun would certainly tell us a great
deal about WIMP dark matter, but unless one also had direct detection or collider evidence,
there would remain many unanswered questions. Are there other celestial bodies that could
provide information about dark matter annihilation? WIMP capture in the Earth would be
very rare, since Earth has a much smaller size and a much smaller escape velocity. In early
papers, Kawasaki et al. [18] and Adler [19] discussed strongly interacting dark matter as
source for heating of gas giant planets, Leane et al. [20] looked at the possibility that dark
matter could be focused by celestial bodies, increasing the rate of annihilation and Leane
and Linden [21] studied gamma ray emission from dark matter annihilation in Jupiter. Very
2
recently, Li and Fan [22] discussed WIMP capture in Jupiter. They also pointed out that
Jupiter is a particularly promising celestial object because it is the largest gas giant and its
core is relatively cool, reducing the evaporation rate. As a result, WIMPs with masses below
the 4 GeV evaporation limit from the Sun could collect in the core. Li and Fan studied the
possibility that the WIMPs could annihilate into long-lived dark mediators which would
convert to electrons and positrons after leaving Jupiter. Current data from the Galileo and
Juno orbiters gave interesting constraints on dark matter models.
These works all considered WIMPs that eventually decay into charged particles. Could
one detect a monoenergetic flux of neutrinos from Jupiter? Obviously, there is no current
detector in orbit that could detect neutrinos, nor is there likely to be for many decades.
But such a detector could encounter a huge flux of neutrinos. The inverse square law alone
would give an enhancement of the square of 1 A.U./RJupiter, which is a factor of five million
relative to DUNE. This could far exceed the reduction due to the smaller size (relative to the
Sun) of Jupiter and the smaller escape velocity. Hopefully by the end of this century robust
exploration of the Jovian system will be underway and the idea of orbiting a neutrino detector
will not be unthinkable. Obviously if dark matter is detected and annihilation into light
quarks is possible, then this type of detector could be helpful. Even if the annihilation into
light quarks is detected at an earlier stage, such a detector could give us direct information
about the Jovian interior. Thus, we feel that it is valuable to study the question of WIMP
annihilation into kaons in Jupiter and the detection of the neutrinos, acknowledging that
such a detection would be decades away.
II. WIMP ANNIHILATION IN JUPITER
A. WIMP population
As WIMPs from the DM halo pass through Jupiter, a portion of them scatter off of
atomic nuclei and enter into bound orbits. While some scatter back out after additional
collisions, the rest remain bound and thermalize in the planet’s core where they annihilate
into Standard Model particles [14,23]. The rate at which the total population of WIMPs
changes with time inside of Jupiter is governed by the differential equation
dNχ(t)
dt =C − ENχ(t)− AN2
χ(t) (2.1)
3
摘要:

MonoenergeticNeutrinosfromWIMPAnnihilationinJupiterGeorgeM.FrenchandMarcSheryHighEnergyTheoryGroup,DepartmentofPhysics,William&Mary,Williamsburg,VA23187-8795,USA(Dated:December14,2022)AbstractWeaklyinteractingmassiveparticles(WIMPs)canbecapturedbytheSunandannihilateinthecore,whichmayresultinproduct...

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