N. D. Scielzo

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.

Improved Limit on Tensor Currents in the Weak Interaction from $^8$Li $β$ Decay

M. T. Burkey [1,2,3], G. Savard [2,3], A. T. Gallant [1], N. D. Scielzo [1,3,4], T. Y. Hirsh [4,3,5], L. Varriano [2,3], G. H. Sargsyan [6], K. D. Launey [6], M. Brodeur [7], D. P. Burdette [7,3], E. Heckmaier [8,1], K. Joerres [6], J. W. Klimes [3], K. Kolos [1], A. Laminack [6], K. G. Leach [9], A. F. Levand [3], B. Longfellow [1,10,3], B. Maaß, S. T. Marley [6], G. E. Morgan [6], P. Mueller [3], R. Orford [3,11], S. W. Padgett [1,3], A. Pérez Galván, J. R. Pierce [2,3], D. Ray [4,3], R. Segel [12], K. Siegl [7], K. S. Sharma [4], B. S. Wang [1]

Abstract

The electroweak interaction in the Standard Model (SM) is described by a pure vector-axial-vector structure, though any Lorentz-invariant component could contribute. In this work, we present the most precise measurement of tensor currents in the low-energy regime by examining the $β$-$\barν$ correlation of trapped $^{8}$Li ions with the Beta-decay Paul Trap. We find $a_{βν} = -0.3325 \pm 0.0013_{stat} \pm 0.0019_{syst}$ at $1σ$ for the case of coupling to right-handed neutrinos $(C_T=-C_T')$, which is consistent with the SM prediction.

Beta-delayed-neutron studies of $^{135,136}$Sb and $^{140}$I performed with trapped ions

B. S. Alan [1,2], S. A. Caldwell [3,4], N. D. Scielzo [1], A. Czeszumska [2], J. A. Clark [4,5], G. Savard [4,3], A. Aprahamian [6], M. T. Burkey [3,4], C. J. Chiara [4,7], J. Harker [4,7], A. F. Levand [4], S. T. Marley [8,6], G. E. Morgan [5,4], J. M. Munson [2], E. B. Norman [2], A. Nystrom [6,4], R. Orford [9,4], S. W. Padgett [1,4,10], A. Perez Galvan, K. S. Sharma [5], K. Siegl [6], S. Y. Strauss [6]

Abstract

Beta-delayed-neutron ($β$n) spectroscopy was performed using the Beta-decay Paul Trap and an array of radiation detectors. The $β$n branching ratios and energy spectra for $^{135,136}$Sb and $^{140}$I were obtained by measuring the time of flight of recoil ions emerging from the trapped ion cloud. These nuclei are located at the edge of an isotopic region identified as having $β$n branching ratios that impact the r-process abundance pattern around the A~130 peak. For $^{135,136}$Sb and $^{140}$I, $β$n branching ratios of 14.6(11)%, 17.6(28)%, and 7.6(28)% were determined, respectively. The $β$n energy spectra obtained for $^{135}$Sb and $^{140}$I are compared with results from direct neutron measurements, and the $β$n energy spectrum for $^{136}$Sb has been measured for the first time.