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The GAmmas from Nuclear Decays Hiding from Investigators (GANDHI) Experiment

1 Pith paper cite this work. Polarity classification is still indexing.

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abstract

We propose a high statistics experiment to search for invisible decay modes in nuclear gamma cascades. A radioactive source (such as $^{60}$Co or $^{24}$Na) that triggers gamma cascades is placed in the middle of a large, hermetically sealed scintillation detector, enabling photon identification with high accuracy. Invisible modes are identified by establishing the absence of a photon in a well-identified gamma cascade. We propose the use of fast scintillators with nanosecond timing resolution, permitting event rates as high as $10^{7}$ Hz. Our analysis of the feasibility of this setup indicates that branching fractions as small as $10^{-12} - 10^{-14}$ can be probed. This experimental protocol benefits from the fact that a search for invisible modes is penalized for weak coupling only in the production of the new particle. If successfully implemented, this experiment is an exquisite probe of particles with mass below $\sim$4 MeV that lie in the poorly constrained supernova "trapping window" that exists between 100 keV - 30 MeV. Such particles have been invoked as mediators between dark matter and nucleons, explain the proton radius and $(g-2)_{\mu}$ anomalies and potentially power the shock wave in type II supernovae. The hadronic axion could also be probed with modifications to the proposed setup.

fields

hep-ph 1

years

2025 1

verdicts

CONDITIONAL 1

representative citing papers

Probing "Continuous Spin" QED with Rare Atomic Transitions

hep-ph · 2025-05-02 · conditional · novelty 6.0

A continuous-spin photon would let forbidden atomic transitions, such as hydrogen 2s to 1s, proceed via single-photon emission, with rates suppressed by powers of ρα/ω and a laboratory bound ρ≲0.1 eV.

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  • Probing "Continuous Spin" QED with Rare Atomic Transitions hep-ph · 2025-05-02 · conditional · none · ref 29 · internal anchor

    A continuous-spin photon would let forbidden atomic transitions, such as hydrogen 2s to 1s, proceed via single-photon emission, with rates suppressed by powers of ρα/ω and a laboratory bound ρ≲0.1 eV.