6533b830fe1ef96bd1296e6a

RESEARCH PRODUCT

Breakdown of the Isobaric Multiplet Mass Equation atA=33,T=3/2

David LunneyJ. SzerypoAlban KellerbauerAlban KellerbauerC. ScheidenbergerS. SchwarzS. SchwarzJens DillingGeorg BollenGeorg BollenR. B. MooreH.-j. KlugeGeorges AudiD. BeckG. SiklerFrank Herfurth

subject

Mass formulaPhysicsMass numberGeneral Physics and AstronomyIsobaric processIon trapAtomic physicsQuadratic form (statistics)Penning trapISOLTRAPMultiplet

description

Mass measurements on ${}^{33,34,42,43}\mathrm{Ar}$ were performed using the Penning trap mass spectrometer ISOLTRAP and a newly constructed linear Paul trap. This arrangement allowed us, for the first time, to extend Penning trap mass measurements to nuclides with half-lives below one second ( ${}^{33}\mathrm{Ar}$: ${T}_{1/2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}174\mathrm{ms}$). A mass accuracy of about ${10}^{\ensuremath{-}7}$ $(\ensuremath{\delta}m\ensuremath{\approx}4\mathrm{keV})$ was achieved for all investigated nuclides. The isobaric multiplet mass equation was checked for the $A\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}33$, $T\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}3/2$ quartet and found to be inconsistent with the generally accepted quadratic form.

https://doi.org/10.1103/physrevlett.87.142501