Petr Balling

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.

Analysis of thermal radiation in ion traps for optical frequency standards

Miroslav Doležal, Petr Balling, Peter B R Nisbet-Jones, Steven A King, Jonathan M Jones, Hugh A Klein, Patrick Gill, Thomas Lindvall, Anders E Wallin, Mikko Merimaa, Christian Tamm, Christian Sanner, Nils Huntemann, Nils Scharnhorst, Ian D Leroux, Piet O Schmidt, Tobias Burgermeister, Tanja E Mehlstäubler, Ekkehard Peik

Abstract

In many of the high-precision optical frequency standards with trapped atoms or ions that are under development to date, the AC Stark shift induced by thermal radiation leads to a major contribution to the systematic uncertainty. We present an analysis of the inhomogeneous thermal environment experienced by ions in various types of ion traps. Finite element models which allow the determination of the temperature of the trap structure and the temperature of the radiation were developed for 5 ion trap designs, including operational traps at PTB and NPL and further optimized designs. Models were refined based on comparison with infrared camera measurement until an agreement of better than 10% of the measured temperature rise at critical test points was reached. The effective temperature rises of the radiation seen by the ion range from 0.8 K to 2.1 K at standard working conditions. The corresponding fractional frequency shift uncertainties resulting from the uncertainty in temperature are in the 10-18 range for optical clocks based on the Sr+ and Yb+ E2 transitions, and even lower for Yb+ E3, In+ and Al+. Issues critical for heating of the trap structure and its predictability were identified and design recommendations developed.