Abstract

A theoretical study of the polarization entanglement of two photons emitted in the decay of metastable ionic states is performed within the framework of density matrix theory and second-order perturbative approach. Particular attention is paid to relativistic and non-dipole effects that become important for medium- and high-ZZ ions. To analyze these effects, the degree of entanglement is evaluated both in the dipole approximation and within the rigorous relativistic theory. Detailed calculations are performed for the two-photon 2s1/2→1s1/22s_{1/2}\to 1s_{1/2} transition in hydrogen-like, as well as for the 1s1/2 2s1/2  1S0→1s1/22  1S01s_{1/2}\, 2s_{1/2} \; {}^1S_0 \to 1s_{1/2}^2 \; {}^1S_0, 1s1/2 2s1/2  3S1→1s1/22  1S01s_{1/2} \, 2s_{1/2} \; {}^3S_1\to 1s_{1/2}^2 \; {}^1S_0 and 1s1/2 2p1/2  3P0→1s1/22  1S01s_{1/2} \, 2p_{1/2} \; {}^3P_0\to 1s_{1/2}^2 \; {}^1S_0 transitions in helium-like ions.

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