December 11, 2024
Facultad de Ciencias Físicas, UCM
Europe/Madrid timezone

First β-decay spectroscopy of Cd132

Dec 11, 2024, 11:20 AM
10m
Aula Magna M1 (Facultad de Ciencias Físicas, UCM)

Aula Magna M1

Facultad de Ciencias Físicas, UCM

Plaza de Ciencias, 1, 28040 Madrid

Speaker

Marcos Llanos Exposito

Description

Isotopes close to the doubly-magic nuclei 132Sn are of strong interest from the point of view
of nuclear structure. Spectroscopic studies are performed with the aim of obtaining a better un-
derstanding of the evolution of shell orbits in nuclei with large N/Z ratios, and providing critical
tests of theoretical models. The information on the nuclear structure and decay properties of n-rich
nuclei in this region may also provide input to calculations for astrophysical r-process.
A new experimental camping was carried out at the ISOLDE facility to study the β-decay
of neutron-rich cadmium isotopes. High intensity Cd (Z = 48) beams were produced after the
fission of a thick UCx target, selectively ionized by the ISOLDE Resonance Ionization Laser Ion
Source (RILIS) and separated in mass using the General Purpose Separator (GPS) ISOLDE mass
separator. A temperature-controlled quartz transfer line was used to ensure purity of the cadmiun
beams [1].The experiment exploited the excellent spectroscopic capabilities of the ISOLDE Decay
Station (IDS). The fast-timing configuration was employed, which included 6 highly efficient clover-
type HPGe detectors, altogether with 2 LaBr3(Ce) and 3 ultra-fast β-plastic detectors arranged in
close geometry.
Direct observation of γ-ray de-excitations and γ-γ coincidences in 132In has been achieved fo-
llowing the β-decay of the 132Cd 0+ ground state (g.s.). The 132In nuclear structure information
is complemented by the β-n decay of 133Cd, providing enhanced statistics. These results expand
those from experiments at RIKEN facility [2,3].
The significantly higher statistics and the possibility of using coincident γ-γ measurements enable
an expanded level scheme and more detailed comparison with shell-model calculations. An inter-
pretation of the level structure is given based on the experimental findings and the particle-hole
configurations arising from core excitations both from the N < 82 and Z < 50 shells, leading to
positive- and negative-parity particle-hole multiplets [2,3].

Presentation materials