2018
DOI: 10.1103/physrevlett.120.103201
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Imaging Optical Frequencies with 100μHz Precision and 1.1μm Resolution

Abstract: We implement imaging spectroscopy of the optical clock transition of lattice-trapped degenerate fermionic Sr in the Mott-insulating regime, combining micron spatial resolution with submillihertz spectral precision. We use these tools to demonstrate atomic coherence for up to 15 s on the clock transition and reach a record frequency precision of 2.5×10^{-19}. We perform the most rapid evaluation of trapping light shifts and record a 150 mHz linewidth, the narrowest Rabi line shape observed on a coherent optical… Show more

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Cited by 179 publications
(124 citation statements)
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“…From this expression, one can see w MF opt is not highly sensitive to variations in the cavity linewidth, κ, but on the contrary it is linearly sensitive to variations on δ c and N. Systematics in the cavity detuning, nevertheless, can be currently controlled at the subhertz level by locking the cavity to a state-of-the-art clock laser [58]. Fluctuations in N can be also suppressed by operating the system in a three dimensional optical lattice in the band or Mott insulator regimes [59] and spectroscopically selecting a fixed region of the atomic array [60].…”
Section: Experimental Realization and Outlookmentioning
confidence: 99%
“…From this expression, one can see w MF opt is not highly sensitive to variations in the cavity linewidth, κ, but on the contrary it is linearly sensitive to variations on δ c and N. Systematics in the cavity detuning, nevertheless, can be currently controlled at the subhertz level by locking the cavity to a state-of-the-art clock laser [58]. Fluctuations in N can be also suppressed by operating the system in a three dimensional optical lattice in the band or Mott insulator regimes [59] and spectroscopically selecting a fixed region of the atomic array [60].…”
Section: Experimental Realization and Outlookmentioning
confidence: 99%
“…The work in this paper is closely tied to the experimental work reported in [34]; we begin with a short summary of the relevant experimental procedures therein. The experiment begins by preparing a degenerate gas of 10 4 -10 5 (fermionic) 87 Sr atoms in a uniform mixture of their ten nuclear spin states and at ∼0.1 of their Fermi temperature (∼10 nanokelvin) [8,40]. This gas is loaded into a primitive cubic optical lattice at the 'magic wavelength' for which both ground ( S 1 0 ) and first-excited ( P 3 0 ) electronic orbital states of the atoms experience the same lattice potential [41].…”
Section: Background and Overviewmentioning
confidence: 99%
“…Only atoms which experience a Zeeman shift that matches the microwave transition frequencies of the narrow transfer window are transferred to the F=7/2 manifold, and are not affected by the optical removal pulse. By imaging the spatial distribution of remaining atoms with fluorescence imaging, we can infer the distribution of the transition frequencies and the magnetic field strengths, a technique referred to as spectral imaging [25].…”
Section: Imaging Magnetic Field Inhomogeneitiesmentioning
confidence: 99%
“…When optimizing our scheme, we observed fast inelastic collisions that only arise when the atoms are in different spin states of the upper hyperfine manifold of the ground state. The frequency sensitivity of the pulses also allowed us to perform spectral imaging [24,25] and visualize our magnetic field gradients directly on a fluorescence image.…”
Section: Introductionmentioning
confidence: 99%