Abstract

This article reports the first optical frequency measurement of the 1S3S1\mathrm{S}-3\mathrm{S} transition in hydrogen. The excitation of this transition occurs at a wavelength of 205 nm which is obtained with two frequency doubling stages of a titanium sapphire laser at 820 nm. Its frequency is measured with an optical frequency comb. The second-order Doppler effect is evaluated from the observation of the motional Stark effect due to a transverse magnetic field perpendicular to the atomic beam. The measured value of the 1S1/2(F=1)3S1/2(F=1)1\mathrm{S}_{1/2}(F=1)-3\mathrm{S}_{1/2}(F=1) frequency splitting is 2922742936.729(13)MHz2 922 742 936.729 (13) \mathrm{MHz} with a relative uncertainty of 4.5×10124.5\times10^{-12}. After the measurement of the 1S2S1\mathrm{S}-2\mathrm{S} frequency, this result is the most precise of the optical frequencies in hydrogen

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