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Towards trapping of hydrogen atoms for computable optical clock applications

O. Amit1,*, D. Taray1, V. Wirthl1, V. Weis1, M. W. Syed1, A. Ozawa1, J. Weitenberg1,2, S. G. Karshenboim1, J. T. M. Walraven3 et al.

L. Maisenbacher4, R. Pohl5, Z. Burkley6, F. Schmid7, T. W. Hänsch1,8, D. C. Yost9, and Th. Udem1,8

  • *Contact author: omer.amit@mpq.mpg.de

Phys. Rev. A 112, 033101 – Published 2 September, 2025

DOI: https://doi.org/10.1103/3bnr-q23f

Abstract

Because of its simple structure, the hydrogen atom is often used as a testbed for quantum electrodynamics. Spectroscopy of trapped atomic samples can greatly improve the accuracy of these tests. Trapping atomic hydrogen in an optical dipole trap or an optical lattice has never been achieved. Only trapping in magnetic fields that lead to large Zeeman shifts has been demonstrated. Standard techniques of atomic physics are difficult to apply to atomic hydrogen. The small mass of the atom and the large photon energy of the 1S-2P cooling transition significantly complicate Doppler cooling. This proposal introduces a photon recoil-assisted loading scheme that uses these properties to our advantage to load atomic hydrogen into an optical dipole trap without laser cooling. The magic wavelength (515 nm) for the 1S-2S clock transition (1.3-Hz natural linewidth) is easily accessible with current laser technology. Since the 1S-2S clock transition can be driven Doppler free, we do not require a very low temperature. Besides improving spectroscopy for fundamental science, such a system can also be used as a “computable” atomic clock that may one day justify the redefinition of the SI second in terms of the Rydberg constant.

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