6533b7ddfe1ef96bd1275124
RESEARCH PRODUCT
Examining the N=28 shell closure through high-precision mass measurements of Ar46–48
Carlo BarbieriCarlo BarbieriM. BreitenfeldRobert WolfRobert WolfKai ZuberSebastian GeorgeAchim SchwenkAchim SchwenkF. HerfurthJason D. HoltV. SomàM. MougeotA. WelkerA. WelkerJ. KartheinJ. KartheinPetr NavrátilA. De RoubinKlaus BlaumD. NeidherrAlexander HerlertMarco RosenbuschLutz SchweikhardVladimir ManeaVladimir ManeaThomas DuguetThomas DuguetFrank WienholtzFrank WienholtzD. LunneyDinko AtanasovDinko Atanasovsubject
PhysicsArgonValence (chemistry)010308 nuclear & particles physicsSHELL modelchemistry.chemical_elementIsotopes of argonRenormalization groupMass spectrometry01 natural sciencesISOLTRAPchemistryAb initio quantum chemistry methods0103 physical sciencesPhysics::Atomic and Molecular ClustersAtomic physics010306 general physicsdescription
The strength of the $N=28$ magic number in neutron-rich argon isotopes is examined through high-precision mass measurements of $^{46\text{--}48}\mathrm{Ar}$, performed with the ISOLTRAP mass spectrometer at ISOLDE/CERN. The new mass values are up to 90 times more precise than previous measurements. While they suggest the persistence of the $N=28$ shell closure for argon, we show that this conclusion has to be nuanced in light of the wealth of spectroscopic data and theoretical investigations performed with the SDPF-U phenomenological shell model interaction. Our results are also compared with ab initio calculations using the valence space in-medium similarity renormalization group and the self-consistent Green's function approaches. Both calculations provide a very good account of mass systematics at and around $Z=18$ and, generally, a consistent description of the physics in this region. This combined analysis indicates that $^{46}\mathrm{Ar}$ is the transition between the closed-shell $^{48}\mathrm{Ca}$ and collective $^{44}\mathrm{S}$.
year | journal | country | edition | language |
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2020-07-01 | Physical Review C |