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      An atomic clock with \(10^{-18}\) instability

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          Abstract

          Atomic clocks have been transformational in science and technology, leading to innovations such as global positioning, advanced communications, and tests of fundamental constant variation. Next-generation optical atomic clocks can extend the capability of these timekeepers, where researchers have long aspired toward measurement precision at 1 part in \(\bm{10^{18}}\). This milestone will enable a second revolution of new timing applications such as relativistic geodesy, enhanced Earth- and space-based navigation and telescopy, and new tests on physics beyond the Standard Model. Here, we describe the development and operation of two optical lattice clocks, both utilizing spin-polarized, ultracold atomic ytterbium. A measurement comparing these systems demonstrates an unprecedented atomic clock instability of \(\bm{1.6\times 10^{-18}}\) after only \(\bm{7}\) hours of averaging.

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          Implementation of Cavity Squeezing of a Collective Atomic Spin

          We squeeze unconditionally the collective spin of a dilute ensemble of laser-cooled rubidium-87 atoms using their interaction with a driven optical resonator. The shape and size of the resulting spin uncertainty region are well described by a simple analytical model [M.H.S., I.D.L., V.V., arXiv:0911.3936] through two orders of magnitude in the effective interaction strength, without free parameters. We deterministically generate states with up to 5.6(6) dB of metrologically relevant spin squeezing on the canonical rubidium-87 hyperfine clock transition.
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            Hyperpolarizability effects in a Sr optical lattice clock

            , , (2005)
            We report the observation of the higher order frequency shift due to the trapping field in a \(^{87}\)Sr optical lattice clock. We show that at the magic wavelength of the lattice, where the first order term cancels, the higher order shift will not constitute a limitation to the fractional accuracy of the clock at a level of \(10^{-18}\). This result is achieved by operating the clock at very high trapping intensity up to \(400 \)kW/cm\(^2\) and by a specific study of the effect of the two two-photon transitions near the magic wavelength.
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              Author and article information

              Journal
              10.1126/science.1240420
              1305.5869

              Quantum physics & Field theory,Optical materials & Optics,Atomic & Molecular physics

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