- Open Access
Optical two-tone time transfer
Phys. Rev. Applied 24, 014001 – Published 1 July, 2025
DOI: https://doi.org/10.1103/9w7h-zzyd
Abstract
Subpicosecond time synchronization can enable future optical timekeeping networks [F. Riehle, Nat. Photonics 11 (1), 25 (2017)], including coherent phased array radar imaging at gigahertz levels [Collaboration, Event Horizon Telescope, Astrophys. J. Lett. 875 (2019)], intercontinental clock comparisons for the redefinition of the second [Dimarcq et al., Metrologia 61 (1), 012001 (2024)], chronometric leveling [Takamoto et al., Nat. Photonics 14 (7), 411 (2020)], and synchronization of remote assets, including future satellite-based optical time standards. With optical clocks now operating on mobile platforms [Roslund et al., Nature 628 (8009), 736 (2024)], free-space synchronization networks with compatible performance and the ability to operate under platform motion are essential to expand the reach of precision timing. Recently, femtosecond-level optical time-transfer techniques have been developed that can operate over hundreds of kilometers despite atmospheric turbulence, signal fade, and dropouts [Giorgetta et al., Nat. Photonics 7, 434 (2013); Caldwell et al., Nature 618 (7966), 721 (2023); Shen et al., Nature 610 (7933), 661 (2022)]. However, practical challenges remain for these pulsed techniques on moving platforms, including dispersion management for variable link lengths and Doppler-induced pulse ambiguities. Continuous-wave techniques overcome these limitations but are prone to femtosecond-level cycle slips during signal fades and dropouts [Gozzard et al., Phys. Rev. Lett. 128, 020801 (2022)]. Here we report an optical time-transfer scheme with femtosecond-level performance that overcomes the practical limitations of dispersion and dropout-induced cycle slips and can also support moving platforms. Importantly, the setup reduces hardware requirements by employing an integrated photonics transceiver and telecom-band lasers that are compatible with full photonic integration. Using this scheme, subfemtosecond synchronization was demonstrated over a free-space link of about 100 m for several hours. Similar performance was demonstrated over a 1-km fiber non-polarization-maintaining link without dispersion compensation. Finally, the link was used to syntonize two iodine optical clocks and then compare them over 4 days. Importantly, the system maintains femtosecond-level performance for received optical power as low as 1 picowatt, compatible with ground-to-satellite link-loss budgets.
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