6533b870fe1ef96bd12cfaab

RESEARCH PRODUCT

Shape isomerism and shape coexistence effects on the Coulomb energy differences in theN=Znucleus66As and neighboringT=1multiplets

S. LeoniS. LeoniJ. J. Valiente-dobónM. P. CarpenterA. BraccoA. BraccoC. A. UrC. A. UrA. GottardoS. M. LenziS. M. LenziB. S. Nara SinghA. M. Bizzeti-sonaA. M. Bizzeti-sonaB. BlankP. G. BizzetiP. G. BizzetiT. MartinezD. SeweryniakC. J. ListerS. ZhuC. J. ChiaraD. MengoniD. MengoniD. R. NapoliW. ReviolD. G. SarantitesKenia Teodoro WiedemannE. FarneaE. FarneaA. GadeaA. PetroviciS. LunardiS. LunardiR. OrlandiO. L. PechenayaKazunari KanekoDimitar TonevE. SahinF. RecchiaF. RecchiaR. WadsworthG. De AngelisJohn P. Greene

subject

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsElectric potential energySHELL modelProlate spheroid01 natural sciencesSymmetry (physics)medicine.anatomical_structureIsospinExcited state0103 physical sciencesmedicineCoulombAtomic physics010306 general physicsNucleus

description

Excited states of the $N=Z=33$ nucleus ${}^{66}$As have been populated in a fusion-evaporation reaction and studied using $\ensuremath{\gamma}$-ray spectroscopic techniques. Special emphasis was put into the search for candidates for the $T=1$ states. A new 3${}^{+}$ isomer has been observed with a lifetime of 1.1(3) ns. This is believed to be the predicted oblate shape isomer. The excited levels are discussed in terms of the shell model and of the complex excited Vampir approaches. Coulomb energy differences are determined from the comparison of the $T=1$ states with their analog partners. The unusual behavior of the Coulomb energy differences in the $A=70$ mass region is explained through different shape components (oblate and prolate) within the members of the same isospin multiplets. This breaking of the isospin symmetry is attributed to the correlations induced by the Coulomb interaction.

https://doi.org/10.1103/physrevc.85.034320