F. G. Kondev

Astrophysical significance of the isomer $^{119m}$Ag demonstrated through direct mass measurement

F. Rivero [1], M. Brodeur [1,2], J. A. Clark, B. Liu [1,2,3,4], G. W. Misch, M. R. Mumpower, W. S. Porter, D. Ray [5,2], G. Savard [2,6,3,5], T. M. Sprouse, A. A. Valverde, D. P. Burdette, A. Cannon [7,8,1], A. T. Gallant, A. M. Houff, K. Kolos [8,2], F. G. Kondev, R. Orford [9], C. Quick [1,5], K. S. Sharma, L. Varriano [10]

Abstract

The abundance of elements heavier than iron produced via the astrophysical rapid-neutron capture process depends sensitively on the atomic mass of the involved nuclei as well as the behavior of a few special types of nuclear isomers called astromers. High-precision mass measurements of $^{119}$Cd, $^{119}$Ag and their respective isomeric states have been performed with the Phase Imaging-Ion Cyclotron Resonance (PI-ICR) method with a precision of $δm/m \approx 10^{-8}$ using the Canadian Penning Trap (CPT). The ground state mass excess, as well as the excitation energy, agrees with recent Penning Trap measurements from JYFLTRAP. Network calculations using these new measurements revealed that, contrary to previous expectations, $^{119m}$Ag behaves as an astromer which significantly affects the population of $^{119}$Ag.

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.

Ground-state and decay properties of neutron-rich 106Nb

A. J. Mitchell [1], R. Orford [2,3], G. J. Lane [1], C. J. Lister [4], P. Copp [4], J. A. Clark [3], G. Savard [3,5], J. M. Allmond [6], A. D. Ayangeakaa [7,8], S. Bottoni [3], M. P. Carpenter [3], P. Chowdhury [4], D. A. Gorelov [3,9], R. V. F. Janssens [7,8], F. G. Kondev [3], U. Patel [1], D. Seweryniak [3], M. L. Smith [1], Y. Y. Zhong [1], S. Zhu [3]

Abstract

The ground-state properties of neutron-rich 106Nb and its beta decay into 106Mo have been studied using the CARIBU radioactive-ion-beam facility at Argonne National Laboratory. Niobium-106 ions were extracted from a 252Cf fission source and mass separated before being delivered as low-energy beams to the Canadian Penning Trap, as well as the X-Array and SATURN beta-decay-spectroscopy station. The measured 106Nb ground-state mass excess of -66202.0(13) keV is consistent with a recent measurement but has three times better precision; this work also rules out the existence of a second long-lived, beta-decaying state in 106Nb above 5 keV in excitation energy. The decay half-life of 106Nb was measured to be 1.097(21) s, which is 8% longer than the adopted value. The level scheme of the decay progeny, 106Mo, has been expanded up to approximately 4 MeV. The distribution of decay strength and considerable population of excited states in 106Mo of J >= 3 emphasises the need to revise the adopted Jpi = 1- ground-state spin-parity assignment of 106Nb; it is more likely to be J => 3.