| Issue |
A&A
Volume 707, March 2026
|
|
|---|---|---|
| Article Number | A295 | |
| Number of page(s) | 4 | |
| Section | Celestial mechanics and astrometry | |
| DOI | https://doi.org/10.1051/0004-6361/202558803 | |
| Published online | 23 March 2026 | |
Two birds with one stone: Simultaneous realization of Lunar Coordinate Time and lunar geoid time with a single orbital clock
1
Purple Mountain Observatory, Chinese Academy of Sciences,
Nanjing
210023,
China
2
School of Astronomy and Space Science, University of Science and Technology of China,
Hefei
230026,
China
3
Shanghai Astronomical Observatory, Chinese Academy of Sciences,
Shanghai
200030,
China
4
School of Astronomy and Space Science, University of Chinese Academy of Sciences,
Beijing
100049,
China
★ Corresponding author: This email address is being protected from spambots. You need JavaScript enabled to view it.
Received:
28
December
2025
Accepted:
21
February
2026
Abstract
Context. There are three options for defining the lunar reference time. Option O1, using Lunar Coordinate Time, has the advantage of simplicity, while options O2 – using the lunar geoid (selenoid) time – and O3 – using an average alignment with Terrestrial Time – have the advantage of convenience for users with instruments on the lunar surface and those using Earth navigation satellite signals, respectively. Clock steering must be performed for all three options. O2 and O3 provide new scalings of spatial coordinates and mass parameters in the Solar System.
Aims. We propose a ‘time-aligned orbit’ in which the readings of an ideal clock in this orbit are equal to the selenoid time in O2; these readings can be converted to Lunar Coordinate Time in O1 via a known linear transformation.
Methods. We show that there exists a time-aligned orbit around the Moon with a semi-major axis of about 1.5 lunar radii that slightly depends on its inclination with respect to the equator of the Moon. We conducted a set of numerical simulations to assess to what extent a clock on these orbits could be used in O2 in a more realistic lunar environment.
Results. The proper time in our simulations de-synchronizes from the selenoid time by up to 190 ns after a year with a frequency offset of 6 × 10−15, which is only 3.75% of the frequency difference in O2 caused by the lunar surface topography. This could be further reduced to 13 ns and 4 × 10−16 if we are able to account for the deviation of the mean orbits in our simulations from the nominal ones.
Conclusions. One can simultaneously realize and use options O1 and O2 by deploying a single clock in the time-aligned orbit. This approach is scalable to other terrestrial planets beyond the Earth–Moon system.
Key words: time
© The Authors 2026
Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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