Probing the Cosmic Neutrino Background through Parametric Fluorescence

We point out that relic neutrinos from the Big Bang may induce the parametric fluorescence in atomic or molecular systems, which offers a novel way to discover cosmic neutrino background. By coherently scattering with molecular energy levels, a massive neutrino can spontaneously "decay" into a lighter neutrino and an infrared signal photon; i.e., ν_{i}+M→ν_{j}+γ_{S}+M, where the molecular state M remains unchanged after the scattering. Because the amplitudes of different radiants are matched in phase, the rate is coherently enhanced and proportional to the squared density of ambient dipoles. When the energy transfer from neutrinos coincides with the energy-level difference, the fluorescence will be on resonance. Near the resonance, the rate is proportional to the square of the coherence time T_{c} of the ensemble. For a nominal target volume of 5 m^{3} (or 5 cm^{3}), the signal rate can reach 1 yr^{-1} for T_{c}=10 ns (or T_{c}=10 μs). This event rate appears to be very promising in consideration of an even longer coherence time that is achievable in solid systems.

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Publication Details

Journal
Physical Review Letters
Published
2026-02-05
DOI
https://doi.org/10.1103/f4zt-bbzv
Primary Topic
Neutrino Physics Research
Type
article
Field-Weighted Citation Impact
0.00
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article

Probing the Cosmic Neutrino Background through Parametric Fluorescence

Guoyuan Huang, Shun Zhou
Physical Review Letters
Neutrino Physics Research
article

Probing the Cosmic Neutrino Background through Parametric Fluorescence

Guoyuan Huang, Shun Zhou
article en

Abstract

We point out that relic neutrinos from the Big Bang may induce the parametric fluorescence in atomic or molecular systems, which offers a novel way to discover cosmic neutrino background. By coherently scattering with molecular energy levels, a massive neutrino can spontaneously "decay" into a lighter neutrino and an infrared signal photon; i.e., ν_{i}+M→ν_{j}+γ_{S}+M, where the molecular state M remains unchanged after the scattering. Because the amplitudes of different radiants are matched in phase, the rate is coherently enhanced and proportional to the squared density of ambient dipoles. When the energy transfer from neutrinos coincides with the energy-level difference, the fluorescence will be on resonance. Near the resonance, the rate is proportional to the square of the coherence time T_{c} of the ensemble. For a nominal target volume of 5 m^{3} (or 5 cm^{3}), the signal rate can reach 1 yr^{-1} for T_{c}=10 ns (or T_{c}=10 μs). This event rate appears to be very promising in consideration of an even longer coherence time that is achievable in solid systems.

Physical Review LettersVol. 136(8)
China University of Geosciences (CN), University of Chinese Academy of Sciences (CN)
Openalex Percentile: Top 99%
Neutrino Physics Research
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