Abstract

The frequency stability of many optical atomic clocks is limited by the coherence of their local oscillator. Here, we present a measurement protocol that overcomes the laser coherence limit. It relies on engineered dynamical decoupling of laser phase noise and near-synchronous interrogation of two clocks. One clock coarsely tracks the laser phase using dynamical decoupling; the other refines this estimate using a high-resolution phase measurement. While the former needs to have a high signal-to-noise ratio, the latter clock may operate with any number of particles. The protocol effectively enables minute-long Ramsey interrogation for coherence times of few seconds as provided by the current best ultrastable laser systems. We demonstrate implementation of the protocol in a realistic proof-of-principle experiment, where we interrogate for 0.5 s at a laser coherence time of 77 ms. Here, a single lattice clock is used to emulate synchronous interrogation of two separate clocks in the presence of artificial laser frequency noise. We discuss the frequency instability of a single-ion clock that would result from using the protocol for stabilisation, under these conditions and for minute-long interrogation, and find expected instabilities of σy(τ) = 8 × 10−16(τ/s)−1/2 and σy(τ) = 5 × 10−17(τ/s)−1/2, respectively.

Highlights

  • The frequency stability of many optical atomic clocks is limited by the coherence of their local oscillator

  • The progress of optical clocks has enabled a multitude of applications that range from testing fundamental symmetries underlying relativity[1,2] and searching for physics beyond the standard model[3,4,5], including dark matter[6,7,8,9,10], to measuring geopotential differences[11,12] and the proposed use for gravitational wave detection[13]

  • The frequency stability of optical clocks is limited by quantum projection noise[21] (QPN) as well as aliased laser frequency noise due to non-continuous observation, which is known as the Dick effect[22,23]

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Summary

Introduction

The frequency stability of many optical atomic clocks is limited by the coherence of their local oscillator. The situation is more complex in optical lattice clocks, which benefit from their lower projection noise (N ≫ 1) Their frequency instability can be improved by reducing projection noise, including the use of spin squeezing[25,26], and by the rejection of the Dick effect using techniques such as synchronous[17] or dead time-free interrogation[19,20]. These are complementary to and can be combined with maximising interrogation time to achieve the best possible frequency stability. The coherence of even the most stable lasers[15] limits interrogation times well short of the excitedstate lifetimes of the most promising clock species[1,27,28,29] and of ultranarrow transitions in several species of highly charged ions[30,31]

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