R. Surman

Mass measurements of neutron-rich nuclides using the Canadian Penning Trap to inform predictions in the $r$-process rare-earth peak region

D. Ray [1,2], N. Vassh [3], B. Liu [4,2,1], A. A. Valverde, M. Brodeur [4,2,1,5,6], J. A. Clark, G. C. McLaughlin, M. R. Mumpower, R. Orford [7,4], W. S. Porter, G. Savard [2,8], K. S. Sharma [1], R. Surman [4], F. Buchinger [9,2], D. P. Burdette, N. Callahan [2,10], A. T. Gallant, D. E. M. Hoff, K. Kolos [10,2], F. G. Kondev, G. E. Morgan [2,11], F. Rivero [4], D. Santiago-Gonzalez [2,10], N. D. Scielzo, L. Varriano [2,8,12], C. M. Weber, G. E. Wilson [11,2,13], X. L. Yan

Abstract

Studies aiming to determine the astrophysical origins of nuclei produced by the rapid neutron capture process ($r$ process) rely on nuclear properties as inputs for simulations. The solar abundances can be used as a benchmark for such calculations, with the $r$-process rare-earth peak (REP) around mass number ($A$) 164 being of special interest due to its presently unknown origin. With the advancement of rare isotope beam production over the last decade and improvement in experimental sensitivities, many of these REP nuclides have become accessible for measurement. Masses are one of the most critical inputs as they impact multiple nuclear properties, namely the neutron-separation energies, neutron capture rates, $β$-decay rates, and $β$-delayed neutron emission probabilities. In this work, we report masses of 20 neutron-rich nuclides (along the Ba, La, Ce, Pr, Nd, Pm, Gd, Dy and Ho isotopic chains) produced at the CAlifornium Rare Isotope Breeder Upgrade (CARIBU) facility at Argonne National Laboratory. The masses were measured with the Canadian Penning trap (CPT) mass spectrometer using the Phase-Imaging Ion-Cyclotron-Resonance (PI-ICR) technique. We then use these new masses along with previously published CPT masses to inform predictions for a Markov Chain Monte Carlo (MCMC) procedure aiming to identify the astrophysical conditions consistent with both solar data and mass measurements. We show that the MCMC responds to this updated mass information, producing refined results for both mass predictions and REP abundances.

Exploring the mass surface near the rare-earth abundance peak via precision mass measurements at JYFLTRAP

M. Vilen [1,2], J. M. Kelly, A. Kankainen [1], M. Brodeur [2], A. Aprahamian [2], L. Canete [1], R. de Groote [1], A. de Roubin [1], T. Eronen [1], A. Jokinen [1,3], I. D. Moore, M. R. Mumpower, D. A. Nesterenko, J. O'Brien, A. Pardo Perdomo [2,1], H. Penttilä, M. Reponen [1], S. Rinta-Antila [1], R. Surman [2]

Abstract

The JYFLTRAP double Penning trap at the Ion Guide Isotope Separator On-Line (IGISOL) facility has been used to measure the atomic masses of 13 neutron-rich rare-earth isotopes. Eight of the nuclides, $^{161}$Pm, $^{163}$Sm, $^{164,165}$Eu, $^{167}$Gd, and $^{165,167,168}$Tb, were measured for the first time. The systematics of the mass surface has been studied via one- and two-neutron separation energies as well as neutron pairing-gap and shell-gap energies. The proton-neutron pairing strength has also been investigated. The impact of the new mass values on the astrophysical rapid neutron capture process has been studied. The calculated abundance distribution results in a better agreement with the solar abundance pattern near the top of the rare-earth abundance peak at around $A\approx165$.