EGU26-19282, updated on 14 Mar 2026
https://doi.org/10.5194/egusphere-egu26-19282
EGU General Assembly 2026
© Author(s) 2026. This work is distributed under
the Creative Commons Attribution 4.0 License.
Poster | Monday, 04 May, 14:00–15:45 (CEST), Display time Monday, 04 May, 14:00–18:00
 
Hall X2, X2.17
ELT: Time transfer by laser pulses
Anja Schlicht1 and the ACES Team*
Anja Schlicht and the ACES Team
  • 1TU Munich, FESG, Munich, Germany (schlicht@bv.tum.de)
  • *A full list of authors appears at the end of the abstract

The Atomic Clock Ensemble in Space (ACES) was launched to the International Space Station (ISS) on 21st of April of this year. Following successful installation on the external payload facility of the Columbus module, the commissioning phase began, which will approximately last until the end of 2025. ACES brought two time transfer methods into orbit: the Microwave Link (MWL) and the European Laser Timing (ELT) link. These two links differ not only in frequency, – one operates in the microwave domain, the other in the optical domain – but also in their detection principle. In this contribution, we introduce the optical pulsed time transfer experiment ELT and compare its measurement principle with that of MWL.

Just like T2L2, ELT is a combination of Satellite Laser Ranging (SLR) and a one-way ranging measurement, in which the laser pulses are time tagged in the ACES timescale. Contrary to T2L2, the complexity of the measurement is not in the space segment but on ground. Although the entire SLR ground segment is available in principle, restrictions exist for ranging to the ISS and the availability of a stable clock signal at these geodetic stations.

The Wettzell Laser Ranging System (WLRS) located at the Geodetic Observatory Wettzell in Germany is the main ground station for the ELT experiment. We describe the steps taken at WLRS to participate in the ELT experiment and the available hardware. We then present the ACES payload and the ELT Data Center, which is responsible for the data processing chain. We highlight the challenges of the data processing based on the first synchronisation measurements between Wettzell and the ACES time scale. Finally, we discuss the objectives of ELT and the benefit optical time transfer will bring for space geodesy and how it fits to the objectives of GGOS. 

ACES Team:

Abgrall M2, Allart E3, Bauch A4, Bize S2, Cacciapuoti L.5, Clairon A2, Crescence P3, Delva P2, Diener WA6, Eckl J7, Enzer DG6, Esnault FX8, Fuijeda M9, Gibble K10, Goujon D11, Guerlin C12, Heimbach F4, Helm A3, Ichikawa R.9, Jetzer P13, Kannanthara J14, Kehrer J3, Kodet J1, Lachaud R3, Laurent P2, Léger B8, Le Poncin-Lafitte C2, Lilley M2, Liu S15, Lorini L2, Lours M2, Marz S1, Mas-sonnet D8, McKelvy J6, Montenbruck O16, Niedermaier T3, Pataraia S5, Patla B17, Peignier T5, Peik E4, Perri A11, Piester D4, Pittet J11, Plumaris M5, Prochazka I18, Rahm J4, Roze J2, Salomon C12, Santarelli G2,19, Savalle E20, Schaefer W15, Schreiber U1, Schwall T15, Schwatke C1, Sekido M9, Shemar S14, Thulliez E8, Tjoelker R6, Tunesi J14, Vollmair P1, Wang Q11, Weinberg S5, Wermuth M16, Weyers S4, Wolf P2, Yu N6

How to cite: Schlicht, A. and the ACES Team: ELT: Time transfer by laser pulses, EGU General Assembly 2026, Vienna, Austria, 3–8 May 2026, EGU26-19282, https://doi.org/10.5194/egusphere-egu26-19282, 2026.