Improved limits for violations of local position invariance from atomic clock comparisons

preprint2021arXivOpen access

Abstract

We compare two optical clocks based on the 2^2S1/2(F=0)→2_{1/2}(F=0)\to {}^2D3/2(F=2)_{3/2}(F=2) electric quadrupole (E2) and the 2^2S1/2(F=0)→2_{1/2}(F=0)\to {}^2F7/2(F=3)_{7/2}(F=3) electric octupole (E3) transition of 171^{171}Yb+^{+} and measure the frequency ratio νE3/νE2=0.932 829 404 530 965 376(32)ν_{\mathrm{E3}}/ν_{\mathrm{E2}}=0.932\,829\,404\,530\,965\,376(32). We determine the transition frequency νE3=642 121 496 772 645.10(8)ν_{E3}=642\,121\,496\,772\,645.10(8) Hz using two caesium fountain clocks. Repeated measurements of both quantities over several years are analyzed for potential violations of local position invariance. We improve by factors of about 20 and 2 the limits for fractional temporal variations of the fine structure constant αα to 1.0(1.1)×10−18/yr1.0(1.1)\times10^{-18}/\mathrm{yr} and of the proton-to-electron mass ratio μμ to −8(36)×10−18/yr-8(36)\times10^{-18}/\mathrm{yr}. Using the annual variation of the Sun's gravitational potential at Earth ΦΦ, we improve limits for a potential coupling of both constants to gravity, (c2/α)(dα/dΦ)=14(11)×10−9(c^2/α) (dα/dΦ)=14(11)\times 10^{-9} and (c2/μ)(dμ/dΦ)=7(45)×10−8(c^2/μ) (dμ/dΦ)=7(45)\times 10^{-8}.

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