Ústav technické a experimentální fyziky Institute of Experimental and Applied Physics

Isolated mixed-symmetry 2+state of the radioactive neutron-rich nuclide 132Te

NázevTitle
Isolated mixed-symmetry 2+state of the radioactive neutron-rich nuclide 132TeIsolated mixed-symmetry 2+state of the radioactive neutron-rich nuclide 132Te
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
T. Stetz, H. Mayr, V. Werner, N. Pietralla, R. Mihai
DOIDOI
10.1103/l6dj-yfz7
Časopis / citaceJournal / citation
PHYSICAL REVIEW C. 2025, 112(3), 034325-1-034325-9. ISSN 2469-9985.
RokYear
2025
JazykLanguage
eng
WoSWoS
001578968400005
ScopusScopus
2-s2.0-105020708314
RIVRIV
RIV/68407700:21670/25:00385953!RIV26-MSM-21670___
ProjektProject
Institucionální podpora na rozvoj výzkumné org.Institucionální podpora na rozvoj výzkumné org.

AbstraktAbstract

The M1 transition strengths between excited 2+ states of the neutron-rich, radioactive nuclide 132Te was studied through direct lifetime measurements using the Doppler-shift attenuation method in a two-neutron transfer reaction on a 130Te target. An unambiguous identification of the lowest-lying mixed-symmetry 2+ state was achieved on the basis of the large B(M 1; 2+2 -* 2+1 ) = 0.18(2) mu 2N transition strength. Results are compared to the shell model, and the analysis of both data and calculations unambiguously identifies the second-excited 2+ state of 132Te as the one-quadrupole phonon mixed-symmetry state of this isotope. A lowering of the energy and B(M 1; 2+ms -* 2+1 ) strength within the N = 80 isotones toward the Z = 50 shell closure is observed, which occurs along with the lowering of the E2 collectivity approaching the magic proton shell.

The M1 transition strengths between excited 2+ states of the neutron-rich, radioactive nuclide 132Te was studied through direct lifetime measurements using the Doppler-shift attenuation method in a two-neutron transfer reaction on a 130Te target. An unambiguous identification of the lowest-lying mixed-symmetry 2+ state was achieved on the basis of the large B(M 1; 2+2 -* 2+1 ) = 0.18(2) mu 2N transition strength. Results are compared to the shell model, and the analysis of both data and calculations unambiguously identifies the second-excited 2+ state of 132Te as the one-quadrupole phonon mixed-symmetry state of this isotope. A lowering of the energy and B(M 1; 2+ms -* 2+1 ) strength within the N = 80 isotones toward the Z = 50 shell closure is observed, which occurs along with the lowering of the E2 collectivity approaching the magic proton shell.