Different mechanism of two-proton emission from proton-rich nuclei $^{23}$Al and $^{22}$Mg
Y.G. Ma, D.Q. Fang, X.Y. Sun, P. Zhou, Y. Togano, N. Aoi, H. Baba,, X.Z. Cai, X.G. Cao, J.G. Chen, Y. Fu, W. Guo, Y. Hara, T. Honda, Z.G. Hu, K., Ieki, Y. Ishibashi, Y. Ito, N. Iwasa, S. Kanno, T. Kawabata, H. Kimura, Y., Kondo, K. Kurita, M. Kurokawa, T. Moriguchi, H. Murakami

TL;DR
This study investigates the decay mechanisms of two proton-rich nuclei, $^{23}$Al and $^{22}$Mg, revealing distinct two-proton emission processes through momentum and angular distribution measurements.
Contribution
It provides experimental evidence of different two-proton emission mechanisms in $^{23}$Al and $^{22}$Mg, highlighting the presence of diproton emission in $^{22}$Mg and sequential decay in $^{23}$Al.
Findings
Peak in $q_{pp}$ and $ heta_{pp}$ for $^{22}$Mg indicating diproton emission
Absence of such peaks in $^{23}$Al suggesting sequential decay
Different emission mechanisms identified for the two nuclei
Abstract
Two-proton relative momentum () and opening angle () distributions from the three-body decay of two excited proton-rich nuclei, namely Al p + p + Na and Mg p + p + Ne, have been measured with the projectile fragment separator (RIPS) at the RIKEN RI Beam Factory. An evident peak at MeV/c as well as a peak in around 30 are seen in the two-proton break-up channel from a highly-excited Mg. In contrast, such peaks are absent for the Al case. It is concluded that the two-proton emission mechanism of excited Mg is quite different from the Al case, with the former having a favorable diproton emission component at a highly excited state and the latter dominated by the sequential decay process.
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