T. Dickel

Prominent bump in the two-neutron separation energies of neutron-rich lanthanum isotopes revealed by high-precision mass spectrometry

A. Jaries [1,2], M. Stryjczyk [1], A. Kankainen [1], T. Eronen [1], O. Beliuskina [1], T. Dickel [3,4], M. Flayol [5], Z. Ge [1,3], M. Hukkanen [1,5], M. Mougeot [1], S. Nikas [1], I. Pohjalainen [1], A. Raggio [1], M. Reponen [1], J. Ruotsalainen [1], V. Virtanen [1]

Abstract

We report on high-precision atomic mass measurements of $^{148\text{-}153}$La and $^{151}$Ce performed with the JYFLTRAP double Penning trap using the Phase-Imaging Ion-Cyclotron-Resonance technique. The masses of $^{152,153}$La were experimentally determined for the first time. We confirm the sharp kink in the two-neutron separation energies at the neutron number ${N=93}$ in the cerium (${Z=58}$) isotopic chain. Our precision mass measurements of the most exotic neutron-rich lanthanum (${Z=57}$) isotopes reveal a sudden increase in two-neutron separation energies from ${N=92}$ to ${N=93}$. Unlike in the cerium isotopic chain, the kink is not sharp but extends to ${N=94}$ forming a prominent bump. The gain in energy is about 0.4 MeV, making it one of the strongest changes in two-neutron separation energies over the whole chart of nuclides, away from nuclear shell closures. The results call for further studies to elucidate the structure of neutron-rich lanthanum isotopes.

Probing the N=104 midshell region for the r process via precision mass spectrometry of neutron-rich rare-earth isotopes with the JYFLTRAP double Penning trap

A. Jaries [1,2], S. Nikas [1], A. Kankainen [1], T. Eronen [1], O. Beliuskina [1], T. Dickel [3,4], M. Flayol [5], Z. Ge [1,3], M. Hukkanen [1,5], M. Mougeot [1], I. Pohjalainen [1], A. Raggio [1], M. Reponen [1], J. Ruotsalainen [1], M. Stryjczyk [1], V. Virtanen [1]

Abstract

We have performed high-precision mass measurements of neutron-rich rare-earth Tb, Dy and Ho isotopes using the Phase-Imaging Ion-Cyclotron-Resonance technique at the JYFLTRAP double Penning trap. We report on the first experimentally determined mass values for $^{169}$Tb, $^{170}$Dy and $^{171}$Dy, as well as the first high-precision mass measurements of $^{169}$Dy and $^{169\text{-}171}$Ho. For $^{170}$Ho, the two long-lived ground and isomeric states were resolved and their mass measured, yielding an isomer excitation energy of $E_\text{exc}=150.8(54)$~keV. In addition, we have performed independent crosschecks of previous Penning-trap values obtained for $^{167\text{,} 168}$Tb and $^{167\text{,} 168}$Dy. We have extended the systematics of two-neutron separation energies to the neutron midshell at $N=104$ in all of the studied isotopic chains. Our updated and new mass measurements provide better mass-related constraints for the neutron-capture reaction rates relevant to the astrophysical rapid neutron capture (r) process. The r-process abundances calculated with the new mass values seem to produce a steeper minimum at A=170 and differ by around 15-30\% from the abundances computed with the Atomic Mass Evaluation 2020 values.

Collision-Induced Dissociation at TRIUMF's Ion Trap for Atomic and Nuclear science

A. Jacobs, C. Andreoiu, J. Bergmann, T. Brunner, T. Dickel, I. Dillmann, E. Dunling, J. Flowerdew, L. Graham, G. Gwinner, Z. Hockenbery, B. Kootte, Y. Lan, K. G. Leach, E. Leistenschneider, E. M. Lykiardopoulou, V. Monier, I. Mukul, S. F. Paul, W. R. Plaß, M. P. Reiter, C. Scheidenberger, R. Thompson, J. L Tracy, C. Will, M. E. Wieser, M. Yavor, J. Dilling [1], A. A. Kwiatkowski

Abstract

The performance of high-precision mass spectrometry of radioactive isotopes can often be hindered by large amounts of contamination, including molecular species, stemming from the production of the radioactive beam. In this paper, we report on the development of Collision-Induced Dissociation (CID) as a means of background reduction for experiments at TRIUMF's Ion Trap for Atomic and Nuclear science (TITAN). This study was conducted to characterize the quality and purity of radioactive ion beams and the reduction of molecular contaminants to allow for mass measurements of radioactive isotopes to be done further from nuclear stability. This is the first demonstration of CID at an ISOL-type radioactive ion beam facility, and it is shown that molecular contamination can be reduced up to an order of magnitude.

Ba$^{2+}$ ion trapping by organic submonolayer: towards an ultra-low background neutrinoless double beta decay detector

P. Herrero-Gómez, J. P. Calupitan, M. Ilyn [1], A. Berdonces-Layunta [1,2], T. Wang [1,2], D. G. de Oteyza [1,2], M. Corso [1,2], R. González-Moreno, I. Rivilla [2,3], B. Aparicio [4,5], A. I. Aranburu, Z. Freixa [5,3], F. Monrabal [2,3,4], F. P. Cossío, J. J. Gómez-Cadenas, C. Rogero [1,2], C. Adams [6,7,8], H. Almazán, V. Alvarez, L. Arazi [9,10], I. J. Arnquist, S. Ayet [11,12], C. D. R. Azevedo, K. Bailey [6], F. Ballester [8,2,13], J. M. Benlloch-Rodríguez, F. I. G. M. Borges, S. Bounasser [7], N. Byrnes [14,15,16], S. Cárcel, J. V. Carrión, S. Cebrián, E. Church [10,13], C. A. N. Conde, T. Contreras [7,17,18,15], A. A. Denisenko, G. Díaz, J. Díaz, T. Dickel [11], J. Escada [13], R. Esteve [8], A. Fahs [7], R. Felkai [9,19], L. M. P. Fernandes, P. Ferrario [2,3,12,17,19], A. L. Ferreira, F. W. Foss, E. D. C. Freitas, J. Generowicz [2], A. Goldschmidt [20,18], D. González-Díaz, R. Guenette [7,21], R. M. Gutiérrez, J. Haefner [7], K. Hafidi [6], J. Hauptman [22,19,18], C. A. O. Henriques, J. A. Hernando Morata, V. Herrero [8], J. Ho [7], Y. Ifergan [9,14], B. J. P. Jones, M. Kekic [18], L. Labarga [23], A. Laing [14], L. Larizgoitia [2], P. Lebrun [24], D. Lopez Gutierrez [7,15], N. López-March, M. Losada [21,19,15,9,2,14,6], R. D. P. Mano, J. Martín-Albo, A. Martínez, G. Martínez-Lema, M. Martínez-Vara, A. D. McDonald, Z. E. Meziani, K. Mistry [14,19,8,15], C. M. B. Monteiro, F. J. Mora, J. Muñoz Vidal, K. Navarro [14], P. Novella [15,14], D. R. Nygren, E. Oblak [2], M. Odriozola-Gimeno [2], B. Palmeiro [18,15], A. Para [24,25], J. Pérez, M. Querol [15], A. Raymond [14,9], A. B. Redwine, J. Renner [18], L. Ripoll [26,21,8], Y. Rodríguez García, J. Rodríguez, L. Rogers [14], B. Romeo [2,25], C. Romo-Luque [15,13,19,9], F. P. Santos, J. M. F. dos Santos, A. Simón, M. Sorel [15], C. Stanford [7,19], J. M. R. Teixeira, P. Thapa [17,8], J. F. Toledo, J. Torrent [2,15,12,17], A. Usón, J. F. C. A. Veloso, T. T. Vuong, R. Webb [27], J. T. White, K. Woodruff [14], N. Yahlali [15]

Abstract

If neutrinos are their own antiparticles, the otherwise-forbidden nuclear reaction known as neutrinoless double beta decay ($ββ0ν$) can occur, with a characteristic lifetime which is expected to be very long, making the suppression of backgrounds a daunting task. It has been shown that detecting (``tagging'') the Ba$^{+2}$ dication produced in the double beta decay ${}^{136}\mathrm{Xe} \rightarrow {}^{136}$Ba$^{+2}+ 2 e + (2 ν)$ in a high pressure gas experiment, could lead to a virtually background free experiment. To identify these \Bapp, chemical sensors are being explored as a key tool by the NEXT collaboration . Although used in many fields, the application of such chemosensors to the field of particle physics is totally novel and requires experimental demonstration of their suitability in the ultra-dry environment of a xenon gas chamber. Here we use a combination of complementary surface science techniques to unambiguously show that Ba$^{+2}$ ions can be trapped (chelated) in vacuum by an organic molecule, the so-called fluorescent bicolour indicator (FBI) (one of the chemosensors developed by NEXT), immobilized on a surface. We unravel the ion capture mechanism once the molecules are immobilised on Au(111) surface and explain the origin of the emission fluorescence shift associated to the trapping of different ions. Moreover, we prove that chelation also takes place on a technologically relevant substrate, as such, demonstrating the feasibility of using FBI indicators as building blocks of a Ba$^{+2}$ detector.

Mass Measurements of Neutron-Rich Gallium Isotopes Refine Production of Nuclei of the First r-Process Abundance Peak in Neutron Star Merger Calculations

M. P. Reiter, S. Ayet San Andrés, S. Nikas [3,4], J. Lippuner [5,6,7], C. Andreoiu [8], C. Babcock [2], B. R. Barquest, J. Bollig [2,9], T. Brunner [2,10], T. Dickel [1,3], J. Dilling [2,11], I. Dillmann [2,12], E. Dunling [2,13], G. Gwinner [14], L. Graham [2], C. Hornung [1], R. Klawitter [2,15], B. Kootte [2,14,12], A. A. Kwiatkowski, Y. Lan [2,11], D. Lascar [2,16,17], K. G. Leach, E. Leistenschneider [2,11,3,4,12,9,1], G. Martínez-Pinedo, J. E. McKay, S. F. Paul, W. R. Plaß, L. Roberts [18], H. Schatz [7,18,19], C. Scheidenberger [1,3], A. Sieverding [3,4,20,2], R. Steinbrügge, R. Thompson [21], M. E. Wieser, C. Will [1], D. Welch [18]

Abstract

We report mass measurements of neutron-rich Ga isotopes $^{80-85}$Ga with TRIUMF's Ion Trap for Atomic and Nuclear science (TITAN). The measurements determine the masses of $^{80-83}$Ga in good agreement with previous measurements. The masses of $^{84}$Ga and $^{85}$Ga were measured for the first time. Uncertainties between $25-48$ keV were reached. The new mass values reduce the nuclear uncertainties associated with the production of A $\approx$ 84 isotopes by the \emph{r}-process for astrophysical conditions that might be consistent with a binary neutron star (BNS) merger producing a blue kilonova. Our nucleosynthesis simulations confirm that BNS merger may contribute to the first abundance peak under moderate neutron-rich conditions with electron fractions $Y_e=0.35-0.38$.

Dawning of the N=32 shell closure seen through precision mass measurements of neutron-rich titanium isotopes

E. Leistenschneider [1,2,3,4], M. P. Reiter, S. Ayet San Andrés, B. Kootte [1,5], J. D. Holt, P. Navrátil, C. Babcock [1], C. Barbieri [6,1], B. R. Barquest, J. Bergmann [3], J. Bollig [1,7], T. Brunner [1,8], E. Dunling [1,9], A. Finlay [1,2], H. Geissel [3,4], L. Graham [1], F. Greiner [3], H. Hergert [10], C. Hornung [3], C. Jesch [3], R. Klawitter [1,11], Y. Lan [1,2], D. Lascar [1,12], K. G. Leach, W. Lippert [3,1,13,7], J. E. McKay, S. F. Paul, A. Schwenk [11,14,15], D. Short [1,16], J. Simonis [17,18,1,19], V. SomÃ, R. Steinbrügge, S. R. Stroberg, R. Thompson [20], M. E. Wieser, C. Will [3], M. Yavor [21], C. Andreoiu [16], T. Dickel [3,4], I. Dillmann [1,13], G. Gwinner [5,3,4], W. R. Plaß, C. Scheidenberger [3,4,1,13], A. A. Kwiatkowski, J. Dilling [1,2]

Abstract

A precision mass investigation of the neutron-rich titanium isotopes $^{51-55}$Ti was performed at TRIUMF's Ion Trap for Atomic and Nuclear science (TITAN). The range of the measurements covers the $N=32$ shell closure and the overall uncertainties of the $^{52-55}$Ti mass values were significantly reduced. Our results confirm the existence of a weak shell effect at $N=32$, establishing the abrupt onset of this shell closure. Our data were compared with state-of-the-art \textit{ab-initio} shell model calculations which, despite very successfully describing where the $N=32$ shell gap is strong, overpredict its strength and extent in titanium and heavier isotones. These measurements also represent the first scientific results of TITAN using the newly commissioned Multiple-Reflection Time-of-Flight Mass Spectrometer (MR-TOF-MS), substantiated by independent measurements from TITAN's Penning trap mass spectrometer.