The Masses of the Nuclei P and S
arXiv:1806.11323 · doi:10.1103/PhysRevC.98.014315
Abstract
Isochronous mass spectrometry has been applied in the storage ring CSRe to measure the masses of the nuclei P and S. The new mass excess value (S) ~keV is 66(52)~keV larger than the result of the previous S(He,He)S reaction measurement in 1973 and a factor of 3.8 more precise. The new result for S, together with those of the isobaric analog states (IAS) in P, Si, and Al, fit well into the quadratic form of the Isobaric Multiplet Mass Equation IMME. The mass excess of P has been remeasured to be P keV. By analyzing the linear and quadratic coefficients of the IMME in the -shell nuclei, it was found that the ratio of the Coulomb radius parameters is and is nearly the same for all isospin multiplets. Such a nearly constant -value, apparently valid for the entire light mass region with , can be used to set stringent constraints on the isovector and isotensor components of the isospin non-conserving forces in theoretical calculations.
arXiv comment7 pages, 4 figures
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Cited by in corpus (8)
- Beta-decay spectroscopy of S
- Particle identification and revolution time corrections for the isochronous mass spectrometry in storage rings
- Characterization of a double Time-Of-Flight detector system for accurate velocity measurement in a storage ring using laser beams
- Charge resolution in the isochronous mass spectrometry and the mass of Co
- Experimentally well-constrained masses of P and S: Implications for studies of explosive binary systems
- Mass measurements for -shell nuclei Ti, Cr, Mn, Fe, Co and Ni
- Beyond Wigner's isobaric multiplet mass equation: Effect of charge-symmetry-breaking interaction and Coulomb polarization
- Improving the resolving power of Isochronous Mass Spectrometry by employing an in-ring mechanical slit