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Advanced Quantum Technologies

Differential Frequency Comparison of Conditionally and Unconditionally Spin‐Squeezed States of an Optical Lattice Clock

Deshui Yu, Xiaobo Xue, Jia Zhang, Shougang Zhang, Jingbiao Chen

Published Feb 13, 2025• 0 citations
Publisher

Abstract

Abstract Optical lattice clocks are the world's most accurate and stable timepieces. Thus far, the differential clock comparison has reached a stability limited by the quantum projection noise of uncorrelated atoms. Overcoming this limit relies on using spin squeezing, where quantum fluctuations of the collective spin undergo a strong suppression in one direction while being enhanced in the conjugation direction. The recent differential comparison of spin‐squeezed clocks mainly employs multiple atomic clouds or sub‐ensembles within one cloud, complicating the clock operation. Here, it is numerically investigated the differential comparison of conditionally and unconditionally spin‐squeezed states of one lattice‐trapped cloud of neutral atoms. The simulation results in a comparison stability of at the averaging time for atoms. The metrological gain reaches dB, primarily limited by the decoherence induced by quantum jumps of intracavity probe photons during quantum non‐demolition measurements. Besides the quantum precision enhancement, our scheme paves the way to using one spin squeezing protocol to appraise the other.

DOI
10.1002/qute.202400491

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•Jan 1, 2023•0 citations
Abstract Optical lattice clocks are the world's most accurate and stable timepieces. Thus far, the differential clock comparison has reached a stability limited by the quantum projection noise of uncorrelated atoms. Overcoming this limit relies on using spin squeezing, where quantum fluctuations of the collective spin undergo a strong suppression in one direction while being enhanced in the conjugation direction. The recent differential comparison of spin‐squeezed clocks mainly employs multiple atomic clouds or sub‐ensembles within one cloud, complicating the clock operation. Here, it is numerically investigated the differential comparison of conditionally and unconditionally spin‐squeezed states of one lattice‐trapped cloud of neutral atoms. The simulation results in a comparison stability of at the averaging time for atoms. The metrological gain reaches dB, primarily limited by the decoherence induced by quantum jumps of intracavity probe photons during quantum non‐demolition measurements. Besides the quantum precision enhancement, our scheme paves the way to using one spin squeezing protocol to appraise the other.
Building scalable quantum systems that demonstrate genuine performance enhancement based on entanglement is a major scientific goal for fields including computing, networking, simulations, and metrology. The tremendous challenge arises from the fragility of entanglement in increasingly larger sized quantum systems. Optical atomic clocks utilizing a large number of atoms have pushed the frontier of measurement science, building on precise engineering of quantum states and control of atomic interactions. However, today's state-of-the-art optical atomic clocks are limited by the quantum projection noise (QPN) defined by many uncorrelated atoms. Pioneering work on producing spin squeezed states of atoms has shown a path towards integrating entanglement into the best performing clocks. However, to directly demonstrate advantage of quantum entanglement in a working clock we must prevent backaction effects that degrade quantum coherence and introduce uncontrolled perturbations, as well as minimize the influence of technical noise arising from the interrogating clock laser. Here we present a new optical clock platform integrated with collective strong-coupling cavity QED for quantum non-demolition (QND) measurement. Optimizing the competition between spin measurement precision and loss of coherence, we measure a Wineland parameter of -1.8(7) dB for 1.9x104^44 atoms, thus verifying the presence of entanglement. Furthermore, a moving lattice allows the cavity to individually address two independent sub-ensembles, enabling us to spin squeeze two clock ensembles successively and compare their performance. This differential comparison between the two squeezed clocks directly verifies enhanced clock stability of 2.0(3) dB below QPN, and 0.6(3) dB above the standard quantum limit (SQL), at the measurement precision level of 10−17^{-17}−17, without subtracting any technical noise contributions.
Many-body entangled states allow precision measurement beyond the standard quantum limit. Yet they have not been effectively exploited in optical lattice clocks except for proof-of-principle demonstrations. Under the current experimental conditions, taking into account the lattice perturbation, atom-atom interactions, and local oscillator noise, we theoretically evaluate the performance of spin-squeezing-based shallow-lattice Yb optical clocks. The numerical simulation shows that the stability of differential frequency comparison between two Yb ensembles in squeezed spin states potentially accesses the ${10}^{\ensuremath{-}19}$ level at the averaging time of 1 s. The resultant Wineland parameter may be as low as ${\ensuremath{\xi}}_{\text{W}}^{2}=0.027$, corresponding to a reduction of averaging time by a factor of 37, and is limited by the collision-induced degradation of spin squeezing. The metrological gain provided by spin squeezing opens up new opportunities for precision measurement and fundamental physics.
Quantum projection noise will soon limit the best achievable precision of optical atomic clocks based on lattice-confined neutral atoms. Squeezing the collective atomic pseudo-spin via measurement of the clock state populations during Ramsey interrogation suppresses the projection noise. We show here that the lattice laser field can be used to perform ideal quantum non-demolition measurements without clock shifts or decoherence and explore the feasibility of such an approach in theory with the lattice field confined in a ring-resonator. Detection of the motional sideband due to the atomic vibration in the lattice wells can yield signal sizes a hundredfold above the projection noise limit.
Optical atomic clocks are a driving force for precision measurements due to the high accuracy and stability demonstrated in recent years. While further improvements to the stability have been envisioned by using entangled atoms, squeezing the quantum mechanical projection noise, evaluating the overall gain must incorporate essential features of an atomic clock. Here, we investigate the benefits of spin squeezed states for clocks operated with typical Brownian frequency noise-limited laser sources. Based on an analytic model of the closed servo-loop of an optical atomic clock, we report here quantitative predictions on the optimal clock stability for a given dead time and laser noise. Our analytic predictions are in good agreement with numerical simulations of the closed servo-loop. We find that for usual cyclic Ramsey interrogation of single atomic ensembles with dead time, even with the current most stable lasers spin squeezing can only improve the clock stability for ensembles below a critical atom number of about one thousand in an optical Sr lattice clock. Even with a future improvement of the laser performance by one order of magnitude the critical atom number still remains below 100,000. In contrast, clocks based on smaller, non-scalable ensembles, such as ion clocks, can already benefit from squeezed states with current clock lasers.
High-bandwidth, high-stability clocks offer unique chances to study fundamental physics beyond simple metrology. Today, the most stable clocks are optical lattice clocks and they can reach a fractional stability of 3.1 × 10^−18 at 1 s averaging time. Their applications are ranging from the redefinition of the SI time unit, the Second, to the possible detection of gravitational waves in space. The stability of optical lattice clocks is primarily limited by quantum projection noise and Dick noise. In this thesis, I present our effort in creating a platform for studying quantum enhanced metrology and its application towards optical lattice clocks. We demonstrated the laser cooling in an optical cavity with Raman-sideband cooling and achieved average vibration number of n = 0.2. We utilized cavity feedback squeezing to demonstrate unitary spin squeezing on magnetic sub-levels of 171Yb, achieving 6.5 dB quantum projection noise reduction over the standard quantum limit (SQL). With coherent optical state transfer by ultra stable laser pulses, we successfully transferred the spin squeezed state from magnetic sub-levels to the optical transition, and demonstrated quantum enhanced metrology in the optical lattice clock for the first time. We achieved 4.4 dB of metrological gain over the SQL, which corresponds to a reduction of the averaging time by a factor of 2.8 in clock operation. Furthermore, we studied quantum enhanced metrology with time-reversal-based protocols. We performed a signal amplification through time-reversed interaction protocol between the ground state magnetic sublevels of 171Yb, achieving the largest sensitivity improvement beyond SQL in any interferometers to date at 11.8dB. Besides that, we experimentally studied the connection between quantum information scrambling, by measuring out-of-time-order correlators (OTOCs), and quantum metrology, by measuring metrological gain. We found these values to agree with each other, and concluded that the time-reversal quantum metrology can saturate the attainable gain from the quantum information scrambling.