TY - JOUR
T1 - Lifetime measurements of states of 35S, 36S 37S, and 38S using the AGATA γ -ray tracking spectrometer
AU - Grocutt, L.
AU - Chapman, R.
AU - Bouhelal, M.
AU - Haas, F.
AU - Goasduff, A.
AU - Smith, J. F.
AU - Lubna, R. S.
AU - Courtin, S.
AU - Bazzacco, D.
AU - Braunroth, T.
AU - Capponi, L.
AU - Corradi, L.
AU - Derkx, X.
AU - Desesquelles, P.
AU - Doncel, M.
AU - Fioretto, E.
AU - Gottardo, A.
AU - Liberati, V.
AU - Melon, B.
AU - Mengoni, D.
AU - Michelagnoli, C.
AU - Mijatović, T.
AU - Modamio, V.
AU - Montagnoli, G.
AU - Montanari, D.
AU - Mulholland, K. F.
AU - Napoli, D. R.
AU - Petrache, C. M.
AU - Pipidis, A.
AU - Recchia, F.
AU - Sahin, E.
AU - Singh, P. P.
AU - Stefanini, A. M.
AU - Szilner, S.
AU - Valiente-Dobón, J. J.
PY - 2022/8/16
Y1 - 2022/8/16
N2 - Lifetimes or lifetime limits of a small number of excited states of the sulfur isotopes with mass numbers A=35, 36, 37, and 38 have been measured using the differential recoil-distance method. The isotopes of sulfur were populated in binary grazing reactions initiated by a beam of S36 ions of energy 225 MeV incident on a thin Pb208 target which was mounted in the Cologne plunger apparatus. The combination of the PRISMA magnetic spectrometer and an early implementation of the AGATA γ-ray tracking array was used to detect γ rays in coincidence with projectile-like nuclear species. Lifetime measurements of populated states were measured within the range from about 1 to 100 ps. The number of states for which lifetime measurements or lifetime limits were possible was limited by statistics. For S35, the lifetime was determined for the first 1/2+ state at 1572 keV; the result is compared with a previous published lifetime value. The lifetime of the 3- state of S36 at 4193 keV was determined and compared with earlier measurements. No previous lifetime information exists for the (6+) state at 6690 keV; a lifetime measurement with large associated error was made in the present work. For S37, the states for which lifetime limits were established were those at 646 keV with Jπ=3/2- and at 2776 keV with Jπ=11/2-; there are no previously published lifetime values for excited states of S37. Finally, a lifetime limit was established for the Jπ=(6+) state of S38 at 3675 keV; no lifetime information exists for this state in the literature. Measured lifetime values were compared with the results of state-of-the-art shell-model calculations based on the PSDPF, SDPF-U, and FSU effective interactions. In addition, nuclear magnetic-dipole and electric-quadrupole moments, branching ratios, mixing ratios, and electromagnetic transition rates, where available, have been compared with shell-model values. The current work suffers from poor statistics; nevertheless, lifetime values and limits have been possible, allowing a useful discussion of the ability of state-of-the-art shell-model calculations to reproduce the experimental results.
AB - Lifetimes or lifetime limits of a small number of excited states of the sulfur isotopes with mass numbers A=35, 36, 37, and 38 have been measured using the differential recoil-distance method. The isotopes of sulfur were populated in binary grazing reactions initiated by a beam of S36 ions of energy 225 MeV incident on a thin Pb208 target which was mounted in the Cologne plunger apparatus. The combination of the PRISMA magnetic spectrometer and an early implementation of the AGATA γ-ray tracking array was used to detect γ rays in coincidence with projectile-like nuclear species. Lifetime measurements of populated states were measured within the range from about 1 to 100 ps. The number of states for which lifetime measurements or lifetime limits were possible was limited by statistics. For S35, the lifetime was determined for the first 1/2+ state at 1572 keV; the result is compared with a previous published lifetime value. The lifetime of the 3- state of S36 at 4193 keV was determined and compared with earlier measurements. No previous lifetime information exists for the (6+) state at 6690 keV; a lifetime measurement with large associated error was made in the present work. For S37, the states for which lifetime limits were established were those at 646 keV with Jπ=3/2- and at 2776 keV with Jπ=11/2-; there are no previously published lifetime values for excited states of S37. Finally, a lifetime limit was established for the Jπ=(6+) state of S38 at 3675 keV; no lifetime information exists for this state in the literature. Measured lifetime values were compared with the results of state-of-the-art shell-model calculations based on the PSDPF, SDPF-U, and FSU effective interactions. In addition, nuclear magnetic-dipole and electric-quadrupole moments, branching ratios, mixing ratios, and electromagnetic transition rates, where available, have been compared with shell-model values. The current work suffers from poor statistics; nevertheless, lifetime values and limits have been possible, allowing a useful discussion of the ability of state-of-the-art shell-model calculations to reproduce the experimental results.
UR - http://www.scopus.com/inward/record.url?scp=85137301155&partnerID=8YFLogxK
U2 - 10.1103/PhysRevC.106.024314
DO - 10.1103/PhysRevC.106.024314
M3 - Article
AN - SCOPUS:85137301155
SN - 2469-9985
VL - 106
JO - Physical Review C
JF - Physical Review C
IS - 2
M1 - 024314
ER -