phenomenon

neutrino dark matter interactions

Interactions between neutrinos and dark matter particles affecting neutrino properties and detection.
24 related articles · 3 formulas

Description

Neutrinos are the lightest known massive particles, streaming through the universe in vast numbers, while dark matter makes up most of the universe's mass yet remains invisible. Their interaction is a key hypothesis: if dark matter particles are light and couple to neutrinos, they could alter neutrino masses, oscillation patterns, or production rates in the early universe. This connection might explain why dark matter's abundance is similar to neutrinos' energy density, a cosmic coincidence.

History

The idea of neutrino-dark matter coupling gained prominence in the 2000s with models of 'secret neutrino interactions' and light dark matter. The concept was popularized by studies of the cosmic neutrino background and its potential to reveal dark matter properties.

How it works

In models where dark matter interacts with neutrinos, the dark matter particles could scatter off neutrinos, changing their momentum or flavor. In the early universe, such interactions would keep neutrinos in thermal contact longer, affecting the number of effective neutrino species and the cosmic microwave background. In the lab, experiments search for anomalous neutrino oscillations or spectral distortions that cannot be explained by standard three-neutrino mixing.

In practice

This research guides the design of next-generation dark matter detectors and neutrino observatories, helping interpret data from experiments like JUNO or Hyper-Kamiokande.

Fun fact

If dark matter interacts with neutrinos, it could make the universe slightly 'foggier' to neutrinos, a subtle effect that might be visible in the cosmic neutrino background from the Big Bang.

Concept graph →

Formulas

$$N = \frac{L}{4\pi d^2} \frac{A t}{\langle E_\nu \rangle}$$
Number of detected neutrinos relates to luminosity, distance, effective area, and exposure time.
What is in the formula
Nvariablenumber of detected neutrino events — count
Lvariableneutrino luminosity of the source — luminosity watt
dvariabledistance from source to detector — distance metre
Avariableeffective area of the detector — area square metre
tvariableexposure time — time second
⟨E_ν⟩variablemean neutrino energy — energy joule
l(ε_1,ε_2)\simeq\frac{4πε_1nd^2}{at\ln(ε_2/ε_1)} · 2606.22387
$$\sigma = \frac{g_1^2 g_2^2 \mu^2}{\pi m^4}$$
Cross section for contact interaction between particles.
What is in the formula
\sigmavariableCross section — cross section square metre
g_1variableCoupling constant of particle 1 — coupling constant joule metre
g_2variableCoupling constant of particle 2 — coupling constant joule metre
\muvariableReduced mass of the two-particle system — mass kilogram
mvariableMass scale (typically the mass of the particles) — mass kilogram
σ^{{el}}_{χp}=\frac{g_q^2g_χ^2μ_{χp}^2}{πm_v^4}=g_d^2\frac{9μ_{χp}^2}{πm_v^4} · 2607.05335v1
$$H_{\text{HFI}} = \boldsymbol{\mu}_I \cdot \mathbf{A} \cdot \mathbf{S}$$
Interaction between nuclear and electron magnetic moments.
What is in the formula
H_{\text{HFI}}variablemagnetic hyperfine interaction Hamiltonian — hamiltonian joule
\boldsymbol{\mu}_Ivariablenuclear magnetic moment — magnetic moment ampere square metre
\mathbf{A}variablehyperfine coupling tensor — tensor joule per ampere square metre
\mathbf{S}variableelectron spin operator — spin operator
\cdotoperatorscalar product of vectors — dot product
h_{{hfi}}^{(m1)}=\boldsymbol{μ}*{t}^{(e)} · 2607.08941

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