F. Abbass

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.

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.