This paper presents a theoretical evaluation of coupled-spin entanglement in the two-proton ($2p$) radioactive emission. The three-body model of ⁶Be with the proton-proton interaction, which is adjusted to reproduce the experimental energy release, is utilized. Time-dependent calculation is performed to compute the coupled-spin state of the emitted two protons. The spin-correlation function S as the Clauser-Horne-Shimony-Holt (CHSH) indicator is evaluated as S 2.65. Namely, the $2p$-spin entanglement beyond the limit of local-hidden-variable (LHV) theory is suggested. This entanglement is sensitive to the proton-proton interaction. The short-lived (broad-width) $2p$~state has the weaker spin entanglement. In parallel, the core-proton interactions do not harm this entanglement during the time-dependent decaying process. The CHSH measurement can be a novel probe into the effective nuclear interaction inside finite systems.
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Tomohiro Oishi (2024) studied this question.
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