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Towards the Limits of Existence of Nuclear Structure: Observation and First spectroscopy of the Isotope $^{31}$K by measuring its three-proton Decay

Authors :
Kostyleva, D.
Mukha, I.
Acosta, L.
Casarejos, E.
Chudoba, V.
Ciemny, A. A.
Dominik, W.
Dueñas, J. A.
Dunin, V.
Espino, J. M.
Estradé, A.
Farinon, F.
Fomichev, A.
Geissel, H.
Gorshkov, A.
Grigorenko, L. V.
Janas, Z.
Kamiński, G.
Kiselev, O.
Knöbel, R.
Krupko, S.
Kuich, M.
Litvinov, Yu. A.
Marquinez-Durán, G.
Martel, I.
Mazzocchi, C.
Nociforo, C.
Ordúz, A. K.
Pfützner, M.
Pietri, S.
Pomorski, M.
Prochazka, A.
Rymzhanova, S.
Sánchez-Benítez, A. M.
Scheidenberger, C.
Simon, H.
Sitar, B.
Stanoiu, M.
Strmen, P.
Szarka, I.
Takechi, M.
Tanaka, Y. K.
Weick, H.
Winkler, M.
Winfield, J. S.
Xu, X.
Zhukov, M. V.
Source :
Phys. Rev. Lett. 123, 092502 (2019)
Publication Year :
2019

Abstract

The most-remote from stability isotope $^{31}$K, which is located four atomic mass units beyond the proton drip line, has been observed. It is unbound in respect to three-proton (${3p}$) emission, and its decays have been detected in flight by measuring trajectories of all decay products using micro-strip detectors. The $3p$-emission processes have been studied by means of angular correlations $^{28}$S+3$p$ and the respective decay vertexes. The energies of the previously-unknown ground and excited states of $^{31}$K have been determined. This provides its $3p$ separation-energy value $S_{3p}$ of $-4.6(2)$ MeV. Upper half-life limits of 10 ps of the observed $^{31}$K states have been derived from distributions of the measured decay vertexes.<br />Comment: 6 pages, 5 figures

Subjects

Subjects :
Nuclear Experiment

Details

Database :
arXiv
Journal :
Phys. Rev. Lett. 123, 092502 (2019)
Publication Type :
Report
Accession number :
edsarx.1905.08154
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevLett.123.092502