Abstract

We report the first operation of a Ra+^{+} optical clock, a promising high-performance clock candidate. The clock uses a single trapped 226^{226}Ra+^{+} ion and operates on the 7s 2S1/2→7s\ ^2S_{1/2}\rightarrow 6d 2D5/26d\ ^2D_{5/2} electric quadrupole transition. By self-referencing three pairs of symmetric Zeeman transitions, we demonstrate a frequency instability of 1.1×10−13\times10^{-13}/τ\sqrtτ, where ττ is the averaging time in seconds. The total systematic uncertainty is evaluated to be Δν/ν=9×10−16{Δν/ ν= 9 \times 10^{-16}}. Using the clock, we realize the first measurement of the ratio of the D5/2D_{5/2} state to the S1/2S_{1/2} state Landé gg-factors: gD/gSg_{D}/g_{S} = 0.5988053(11). A Ra+^{+} optical clock could improve limits on the time variation of the fine structure constant, α˙/α\dot α/ α, in an optical frequency comparison. The ion also has several features that make it a suitable system for a transportable optical clock.

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