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      Single-Ion Atomic Clock with \(3\times10^{-18}\) Systematic Uncertainty

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          Abstract

          We experimentally investigate an optical frequency standard based on the \(^2S_{1/2} (F=0)\to {}^2F_{7/2} (F=3)\) electric octupole (\textit{E}3) transition of a single trapped \(^{171}\)Yb\(^+\) ion. For the spectroscopy of this strongly forbidden transition, we utilize a Ramsey-type excitation scheme that provides immunity to probe-induced frequency shifts. The cancellation of these shifts is controlled by interleaved single-pulse Rabi spectroscopy which reduces the related relative frequency uncertainty to \(1.1\times 10^{-18}\). To determine the frequency shift due to thermal radiation emitted by the ion's environment, we measure the static scalar differential polarizability of the \textit{E}3 transition as \(0.888(16)\times 10^{-40}\) J m\(^2\)/V\(^2\) and a dynamic correction \(\eta(300~\text{K})=-0.0015(7)\). This reduces the uncertainty due to thermal radiation to \(1.8\times 10^{-18}\). The residual motion of the ion yields the largest contribution \((2.1\times 10^{-18})\) to the total systematic relative uncertainty of the clock of \(3.2\times 10^{-18}\).

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          Optical Dipole Traps for Neutral Atoms

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            Systematic evaluation of an atomic clock at 2 × 10−18 total uncertainty

            The pursuit of better atomic clocks has advanced many research areas, providing better quantum state control, new insights in quantum science, tighter limits on fundamental constant variation and improved tests of relativity. The record for the best stability and accuracy is currently held by optical lattice clocks. Here we take an important step towards realizing the full potential of a many-particle clock with a state-of-the-art stable laser. Our 87Sr optical lattice clock now achieves fractional stability of 2.2 × 10−16 at 1 s. With this improved stability, we perform a new accuracy evaluation of our clock, reducing many systematic uncertainties that limited our previous measurements, such as those in the lattice ac Stark shift, the atoms' thermal environment and the atomic response to room-temperature blackbody radiation. Our combined measurements have reduced the total uncertainty of the JILA Sr clock to 2.1 × 10−18 in fractional frequency units.
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              Cryogenic optical lattice clocks

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                Author and article information

                Journal
                2016-02-11
                Article
                10.1103/PhysRevLett.116.063001
                1602.03908
                597fc18c-be99-45ba-80e4-e10ceb9ad965

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                Phys. Rev. Lett. 116, 063001 (2016)
                5 pages, 4 figures
                physics.atm-clus physics.atom-ph

                Atomic & Molecular physics
                Atomic & Molecular physics

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