1. Different mechanism of two-proton emission from proton-rich nuclei Al and Mg
- Author
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Ma, Y.G., Fang, D.Q., Sun, X.Y., Zhou, P., Togano, Y., Aoi, N., Baba, H., Cai, X.Z., Cao, X.G., Chen, J.G., Fu, Y., Guo, W., Hara, Y., Honda, T., Hu, Z.G., Ieki, K., Ishibashi, Y., Ito, Y., Iwasa, N., Kanno, S., Kawabata, T., Kimura, H., Kondo, Y., Kurita, K., Kurokawa, M., Moriguchi, T., Murakami, H., Ooishi, H., Okada, K., Ota, S., Ozawa, A., Sakurai, H., Shimoura, S., Shioda, R., Takeshita, E., Takeuchi, S., Tian, W.D., Wang, H.W., Wang, J.S., Wang, M., Yamada, K., Yamada, Y., Yasuda, Y., Yoneda, K., Zhang, G.Q., and Motobayashi, T.
- Abstract
Two-proton relative momentum (qpp) and opening angle (θpp) distributions from the three-body decay of two excited proton-rich nuclei, namely Al23→p+p+Na21 and Mg22→p+p+Ne20, have been measured with the projectile fragment separator (RIPS) at the RIKEN RI Beam Factory. An evident peak at qpp∼20 MeV/c as well as a peak in θpp around 30° are seen in the two-proton break-up channel from a highly-excited 22Mg. In contrast, such peaks are absent for the 23Al case. It is concluded that the two-proton emission mechanism of excited 22Mg is quite different from the 23Al case, with the former having a favorable diproton emission component at a highly excited state and the latter dominated by the sequential decay process.
- Published
- 2015