Christian Lisdat

A high-stability optical clock based on a continuously ground-state cooled Al$^+$ ion without compromising its accuracy

Fabian Dawel [1,2], Lennart Pelzer [1], Kai Dietze [1,2], Johannes Kramer [1,2], Marek Hild [1], Steven A. King [1,3], Nicolas C. H. Spethmann, Joshua Klose [1], Kilian Stahl [1], Sören Dörscher, Erik Benkler [1], Christian Lisdat [1], Sergey G. Porsev [4], Marianna S. Safronova [4], Piet O. Schmidt [1,2]

Abstract

Single ion optical clocks have shown systematic frequency uncertainties below $10^{-18}$, but typically require more than one week of averaging to achieve a corresponding statistical uncertainty. This time can be reduced with longer probe times, but comes at the cost of a higher time-dilation shift due to motional heating of the ions in the trap. We show that sympathetic ground-state cooling using electromagnetically-induced transparency (EIT) of an \Al clock ion via a co-trapped \Ca ion during clock interrogation suppresses the heating of the ions. \Al can be kept close to the motional ground state, independent from the chosen interrogation time, at a relative time dilation shift of $(-1.69\pm0.20)\times10^{-18}$. The \Ca cooling light introduces an additional light shift on the \Al clock transition of $(-9.27\pm 1.03)\times10^{-18}$. We project that the uncertainty of this light shift can be further reduced by nearly an order of magnitude. This sympathetic cooling enables seconds of interrogation time with $10^{-19}$ motional and cooling laser-induced uncertainties for \Al and can be employed in other ion clocks as well.

Guidelines for developing optical clocks with $10^{-18}$ fractional frequency uncertainty

Moustafa Abdel-Hafiz [1], Piotr Ablewski [2], Ali Al-Masoudi [1,3], Héctor Ã\udc81lvarez Martínez, Petr Balling [4], Geoffrey Barwood [5], Erik Benkler [1], Marcin Bober [2], Mateusz Borkowski [2], William Bowden [5,2], Roman CiuryÅ‚o, Hubert Cybulski [2], Alexandre Didier [1,4], Miroslav Doležal, Sören Dörscher, Stephan Falke [1], Rachel M. Godun [5], Ramiz Hamid [6], Ian R. Hill [5], Richard Hobson [5], Nils Huntemann [1], Yann Le Coq [7], Rodolphe Le Targat [7], Thomas Legero [1], Thomas Lindvall [8], Christian Lisdat [1,7], Jérôme Lodewyck, Helen S. Margolis [5,1], Tanja E. Mehlstäubler, Ekkehard Peik [1], Lennart Pelzer [1,9], Marco Pizzocaro [10], Benjamin Rauf [10], Antoine Rolland [5], Nils Scharnhorst [1,9], Marco Schioppo [5], Piet O. Schmidt [1,9], Roman Schwarz [1,6,11], ÇaÄŸrı Åženel, Nicolas Spethmann [1], Uwe Sterr [1], Christian Tamm [1], Jan W. Thomsen [12], Alvise Vianello [5,2,8], MichaÅ‚ Zawada

Abstract

There has been tremendous progress in the performance of optical frequency standards since the first proposals to carry out precision spectroscopy on trapped, single ions in the 1970s. The estimated fractional frequency uncertainty of today's leading optical standards is currently in the $10^{-18}$ range, approximately two orders of magnitude better than that of the best caesium primary frequency standards. This exceptional accuracy and stability is resulting in a growing number of research groups developing optical clocks. While good review papers covering the topic already exist, more practical guidelines are needed as a complement. The purpose of this document is therefore to provide technical guidance for researchers starting in the field of optical clocks. The target audience includes national metrology institutes (NMIs) wanting to set up optical clocks (or subsystems thereof) and PhD students and postdocs entering the field. Another potential audience is academic groups with experience in atomic physics and atom or ion trapping, but with less experience of time and frequency metrology and optical clock requirements. These guidelines have arisen from the scope of the EMPIR project "Optical clocks with $1 \times 10^{-18}$ uncertainty" (OC18). Therefore, the examples are from European laboratories even though similar work is carried out all over the world. The goal of OC18 was to push the development of optical clocks by improving each of the necessary subsystems: ultrastable lasers, neutral-atom and single-ion traps, and interrogation techniques. This document shares the knowledge acquired by the OC18 project consortium and gives practical guidance on each of these aspects.