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Entangled two-proton emission from 16Ne and its sensitivity to diproton correlation

Tomohiro Oishi, Masaaki Kimura

Abstract

We discuss how the spin correlation, which reflects the quantum entanglement between two fermions, can serve as a probe of diproton correlation in the two-proton ($2p$) emission. We investigated the 16Ne nucleus using the time-dependent three-body (14O + 2p) model, and found that the $2p$-spin correlation exceeded the limit of local-hidden-variable (LHV) theory when the initial state had a spin-singlet diproton configuration. In contrast, for other configurations, it was remarkably reduced. This suggests that a strong initial diproton correlation is essential to generate a spin correlation nearly identical to that of a pure spin-singlet diproton. Such sensitivity indicates that $2p$-spin correlation can serve as a sensitive probe of diproton configurations, which could facilitate future studies on quantum entanglement and spin-dependent phenomena in atomic nuclei as well as in broader multi-fermion systems.

Entangled two-proton emission from 16Ne and its sensitivity to diproton correlation

Abstract

We discuss how the spin correlation, which reflects the quantum entanglement between two fermions, can serve as a probe of diproton correlation in the two-proton () emission. We investigated the 16Ne nucleus using the time-dependent three-body (14O + 2p) model, and found that the -spin correlation exceeded the limit of local-hidden-variable (LHV) theory when the initial state had a spin-singlet diproton configuration. In contrast, for other configurations, it was remarkably reduced. This suggests that a strong initial diproton correlation is essential to generate a spin correlation nearly identical to that of a pure spin-singlet diproton. Such sensitivity indicates that -spin correlation can serve as a sensitive probe of diproton configurations, which could facilitate future studies on quantum entanglement and spin-dependent phenomena in atomic nuclei as well as in broader multi-fermion systems.

Paper Structure

This paper contains 15 equations, 6 figures.

Figures (6)

  • Figure 1: Spin correlation of the pure $S_{12}=0$ and spherical $S_{12}=1$ states. The limit of LHV theory reads $S(\Phi) =2$1969CHSH.
  • Figure 2: Density distribution of $2p$ state at $t=0$ for $^{16}$Ne. For convention of plotting variables, see Refs. 2014Oishi2017Oishi2023Pfutzner_rev. Same distributions in the sequential and angular-symmetric cases are also plotted.
  • Figure 3: Decaying probability $P_{\rm decay} (t)$ from the diproton-dominant initial state of $^{16}$Ne. The $S_{12}=0$ ratio is also plotted. Same results in the sequential and angular-symmetric cases are compared. Note that their time scales are different.
  • Figure 4: (Top) Spin correlations $S(\Phi = \pi /4)$ calculated for the time-dependent decaying states of $^{16}$Ne. In the sequential case, its time is scaled by $10$, due to the short life time. (Bottom) $S(\Phi)$ evaluated when $P_{\rm decay} (t) \cong 0.0068$.
  • Figure 5: Time-dependent decaying-density distributions in the $2p$ emission of $^{16}$Ne. See Ref. 2025Oishi_16Ne for plotting methods.
  • ...and 1 more figures