6533b839fe1ef96bd12a6e0f

RESEARCH PRODUCT

Spectroscopy of Cd98 by two-nucleon removal from In100

Joochun ParkCenxi YuanK. WimmerF. BrowneI. ZanonS. T. WangLuis Sarmiento PicoSidong ChenP LiangT. LokotkoAlessandra CorsiRyo TaniuchiZhengtai LiuK. KokubunT. KoiwaJenny LeeD. BrugnaraHiroyoshi SakuraiJoakim CederkällP. DoornenbalJinjia LiuSun ZhipengW. XianP. LiShan JinJ. GerlG. HäfnerShigeru KubonoAlejandro AlgoraM. L. CortésM. GórskaP. Koseoglou

subject

PhysicsProton010308 nuclear & particles physicsSpace (mathematics)01 natural sciences7. Clean energyAtomic orbitalYield (chemistry)0103 physical sciencesLevel structureAtomic physics010306 general physicsSpectroscopyNucleonExcitation

description

Low-lying states of Cd-98 have been populated by the two-nucleon removal reaction (In-100, Cd-98+gamma) and studied using in-beam gamma-ray spectroscopy at the Radioactive Isotope Beam Factory at RIKEN. Two new gamma transitions were identified and assigned as decays from a previously unknown state. This state is suggested to be based on a pi 1g(/9/2)(-1)2p(1/2)(-2) configuration with J(pi) = 5(-). The present observation extends the systematics of the excitation energies of the first 5(-) state in N = 50 isotones toward Sn-100. The determined energy of the 5(- )state in Cd-98 continues a smooth trend along the N = 50 isotones. The systematics are compared with shell-model calculations in different model spaces. Good agreement is achieved when considering a model space consisting of the pi(1f(5/2), 2p(3/2), 2p(1/2), 1g(9/2)) orbitals. The calculations with a smaller model space omitting the orbitals below the Z = 38 subshell could not reproduce the experimental energy difference between the ground and first 5(-) states in N = 50 isotones, because proton excitations across Z = 38 subshell yield a large amount of correlation energy that lowers the ground states. (Less)

https://doi.org/10.1103/physrevc.104.024302