Precision laser spectroscopy of trapped ions has proven to be a precise tool not only to build high-precision optical clocks but also to find applications in quantum computing [1,2]. In addition, the remarkable degree of control makes table-top trapped ion systems competitive with large-scale accelerator facilities for finding new physics [3]. Scaling up these systems from one to tens of ions, forming so called Coulomb crystals, requires fast and reliable imaging of individually resolved emitters that are separated by a few micrometers. We use Ytterbium ions due to their large sensitivity for new physics [4,5]. The ions scatter light near a wavelength of 370 nm, where the detection efficiency of standard camera sensors begins to drop.
Experiment
We trap Ytterbium ions in a precision-machined radiofrequency Paul trap [6]. The ions are produced via photoionization of neutral Ytterbium from an effusive oven and imaged onto the EMCCD camera iXon DU897 UCS-BB from Andor with a magnification of 24. The back-illuminated sensor variant BB has proven to have an enhanced quantum efficiency over other models in the near-UV and blue wavelength regime. In our experiment, we excite the ions into the metastable electronic F-State, which is extremely sensitive to a potential Lorentz violation. A complex sequence of radiofrequency pulses mixes the different spin states in the F-manifold, such that a potential violation signal can be picked up. A violation signal would manifest in a variation of the state-population in these states over the sidereal day [Figure 1].

Figure 1: Superposition of electronic spin states in the F-manifold of Yb+. While the earth rotates over the Sidereal day, a potential violation of Lorentz symmetry would manifest in a periodic phase shift between the states that is transgerred to a shift in state populations.
After the sequence, we de-excite the ion back to the electronic ground state, where it can scatter photons near 370 nm wavelength. To analyze the success of the de-excitation, we are interested in whether individual ions are fluorescing or not when illuminated with the 370 nm detection laser, referred to as state-detection. The latter case corresponds to the ions still being in the metastable electronic F-state and thus not able to scatter light near a wavelength of 370 nm, which hints to a violation of local Lorentz invariance. Thus, it is of high importance for us that the signal-to-noise ratio of the camera sensors is large to prevent false-positive and false-negative signals. At the same time, fast detection within a few milliseconds is required to keep the detection overhead in our measurements low. A typical image of a linear ten ion crystal is shown in Figure 2, where eight ions are in the bright state and two ions are in the metastable F-state, appearing as gaps in the crystal.

Figure 2: False-color image of a linear Coulomb crystal composed of ten Yb+ ions, eight of them fluorescing near 370nm wavelength.
References
- A. D. Ludlow et al., Rev. Mod. Phys 87, 637 (2015)
- I. Pogorelov et al., PRX Quantum 2, 020343 (2021)
- M. S. Safronova et al., Rev. Mod. Phys. 90, 025008 (2018)
- R. Shaniv et al., Phys. Rev. Lett., 120, 103202 (2018)
- J. C. Berengut et al, Phys. Rev. Lett., 120, 091801 (2018)
- J. Keller et al., Phys. Rev. Applied, 11, 011002 (2019)
Contact
Prof. Dr. Tanja Mehlstäubler
QuaCCS - Quantum Clocks and Complex Systems
QUEST (Institute for Quantum Metrology)
Physikalisch-Technische Bundesanstalt (PTB)
Bundesallee 100
38116 Braunschweig
Germany
Phone: +49 (531) 592 4710
Email: tanja.mehlstaeubler@ptb.de
Web: http://www.quantummetrology.de/quaccs/home/