C. Will

Orders of Magnitude Improved Cyclotron-Mode Cooling for Non-Destructive Spin Quantum Transition Spectroscopy with Single Trapped Antiprotons

B. M. Latacz [1,2], M. Fleck [1,3,2,4], J. I. Jaeger, G. Umbrazunas [1,5], B. P. Arndt [1,4,6], S. R. Erlewein [1,4], E. J. Wursten [1], J. A. Devlin [1,2], P. Micke [1,2,4], F. Abbass [7], D. Schweitzer [7], M. Wiesinger [4], C. Will [4], H. Yildiz [7], K. Blaum [4], Y. Matsuda [3], A. Mooser [4], C. Ospelkaus [8,9], A. Soter [5], W. Quint [6], J. Walz [7,10], Y. Yamazaki [1], C. Smorra [1,7], S. Ulmer [1,11]

Abstract

We demonstrate efficient sub-thermal cooling of the modified cyclotron mode of a single trapped antiproton and reach particle temperatures $T_+=E_+/k_\text{B}$ below $200\,$mK in preparation times shorter than $500\,$s. This corresponds to the fastest resistive single-particle cyclotron cooling to sub-thermal temperatures ever demonstrated. By cooling trapped particles to such low energies, we demonstrate the detection of antiproton spin transitions with an error-rate $<0.000025$, more than three orders of magnitude better than in previous best experiments. This method will have enormous impact on multi-Penning-trap experiments that measure magnetic moments with single nuclear spins for tests of matter/antimatter symmetry, high-precision mass-spectrometry, and measurements of electron $g$-factors bound to highly-charged ions that test quantum electrodynamics.

BASE-STEP: A transportable antiproton reservoir for fundamental interaction studies

C. Smorra [1,2], F. Abbass [1], M. Bohman [2,3], Y. Dutheil [4], A. Hobl [5], D. Popper [1], B. Arndt [2,3,6], B. B. Bauer [1,2], J. A. Devlin [2,4], S. Erlewein [2,3,4], M. Fleck [2,3,4], J. I. Jäger, B. M. Latacz [2,4], P. Micke [3,4], M. Schiffelholz [7,8], G. Umbrazunas [2,9], M. Wiesinger [3], C. Will [3], E. Wursten [2,4], H. Yildiz [1], K. Blaum [3], Y. Matsuda [10], A. Mooser [3], C. Ospelkaus [7,8], W. Quint [6], A. Soter [9], J. Walz [1,11], Y. Yamazaki [2], S. Ulmer [2,12]

Abstract

Currently, the only worldwide source of low-energy antiprotons is the AD/ELENA facility located at CERN. To date, all precision measurements on single antiprotons have been conducted at this facility and provide stringent tests of the fundamental interactions and their symmetries. However, the magnetic field fluctuations from the facility operation limit the precision of upcoming measurements. To overcome this limitation, we have designed the transportable antiproton trap system BASE-STEP to relocate antiprotons to laboratories with a calm magnetic environment. We anticipate that the transportable antiproton trap will facilitate enhanced tests of CPT invariance with antiprotons, and provide new experimental possibilities of using transported antiprotons and other accelerator-produced exotic ions. We present here the technical design of the transportable trap system. This includes the transportable superconducting magnet, the cryogenic inlay consisting of the trap stack and the detection systems, and the differential pumping section to suppress the residual gas flow into the cryogenic trap chamber.

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.

Sympathetic cooling schemes for separately trapped ions coupled via image currents

C. Will [1], M. Bohman [1,2], T. Driscoll [3], M. Wiesinger [1,2], F. Abbass [4], M. J. Borchert [2,5,6], J. A. Devlin [2,7], S. Erlewein [2,7], M. Fleck [2,8], B. Latacz [2], R. Moller [4], A. Mooser [1], D. Popper [4], E. Wursten [1,2,7], K. Blaum [1], Y. Matsuda [8], C. Ospelkaus [5,6], W. Quint [9], J. Walz [4,10], C. Smorra [2,4], S. Ulmer [2]

Abstract

Cooling of particles to mK-temperatures is essential for a variety of experiments with trapped charged particles. However, many species of interest lack suitable electronic transitions for direct laser cooling. We study theoretically the remote sympathetic cooling of a single proton with laser-cooled $^9$Be$^+$ in a double-Penning-trap system. We investigate three different cooling schemes and find, based on analytical calculations and numerical simulations, that two of them are capable of achieving proton temperatures of about 10 mK with cooling times on the order of 10 s. In contrast, established methods such as feedback-enhanced resistive cooling with image-current detectors are limited to about 1 K in 100 s. Since the studied techniques are applicable to any trapped charged particle and allow spatial separation between the target ion and the cooling species, they enable a variety of precision measurements based on trapped charged particles to be performed at improved sampling rates and with reduced systematic uncertainties.

Sympathetic cooling of a trapped proton mediated by an LC circuit

M. Bohman [1], V. Grunhofer, C. Smorra, M. Wiesinger [1], C. Will [1], M. J. Borchert [4], J. A. Devlin, S. Erlewein, M. Fleck, S. Gavranovic, J. Harrington [1], B. Latacz, A. Mooser [1], D. Popper, E. Wursten, K. Blaum [1], Y. Matsuda, C. Ospelkaus [4], W. Quint, J. Walz, S. Ulmer

Abstract

Efficient cooling of trapped charged particles is essential to many fundamental physics experiments, to high-precision metrology, and to quantum technology. Until now, sympathetic cooling has required close-range Coulomb interactions, but there has been a sustained desire to bring laser-cooling techniques to particles in macroscopically separated traps, extending quantum control techniques to previously inaccessible particles such as highly charged ions, molecular ions and antimatter. Here we demonstrate sympathetic cooling of a single proton using laser-cooled Be+ ions in spatially separated Penning traps. The traps are connected by a superconducting LC circuit that enables energy exchange over a distance of 9 cm. We also demonstrate the cooling of a resonant mode of a macroscopic LC circuit with laser-cooled ions and sympathetic cooling of an individually trapped proton, reaching temperatures far below the environmental temperature. Notably, as this technique uses only image-current interactions, it can be easily applied to an experiment with antiprotons, facilitating improved precision in matter-antimatter comparisons and dark matter searches.

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.