Atomic clock comparisons with a 3e-16 uncertainty via geostationary satellites

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dc.identifier.uri http://dx.doi.org/10.15488/11330
dc.identifier.uri https://www.repo.uni-hannover.de/handle/123456789/11417
dc.contributor.author Riedel, Franziska eng
dc.date.accessioned 2021-09-20T09:25:17Z
dc.date.available 2021-09-20T09:25:17Z
dc.date.issued 2021
dc.identifier.citation Riedel, Franziska: Atomic clock comparisons with a 3e-16 uncertainty via geostationary satellites. Hannover : Gottfried Wilhelm Leibniz Universität, Diss., 2021, VIII, 138 S. DOI: https://doi.org/10.15488/11330 eng
dc.description.abstract Optical clocks are superior to all other clocks, reaching 1e-18 in their uncertainty. This makes them not only attractive for the field of fundamental research, like testing General Relativity or examining the variance of fundamental constants, but marks them also as potential candidates for the new definition of the second. An essential step towards that direction is the possibility to carry out comparisons of optical clocks at remote sites to have consistency checks of clocks constructed mostly independently by different groups. Satellite-based techniques offer the possibility of simultaneous comparisons over a large variety of baselines. Their instability, however, has been demonstrated to be in the low 1e-15 range at 1 d averaging time for most measurements. In case of two-way satellite time and frequency transfer (TWSTFT), the instability is limited by the modulation bandwidth of the signal. For this work, the full bandwidth of 20 Mchip/s of the commonly used TWSTFT equipment, a SATRE modem, is employed, providing a potential improvement of a factor of 20 with respect to the currently performed TWSTFT measurements for the time scale comparisons contributing to TAI. This technique is used in this work to compare five optical clocks and six microwave fountain clocks located at four different European metrology institutes simultaneously over a period of 26 d. In order to prepare this measurement, extensive studies on the SATRE modem are carried out and presented, and other aspects that need to be taken into account for TWSTFT measurements with low instabilities are discussed, such as atmospheric delays, geometric and relativistic effects and laboratory and roof station setups. The link instability of TWSTFT during the measurement campaign is presented, and compared to the instability of GPS Precise Point Positioning, that is implemented as an additional, independent comparisons technique for the campaign. Relative frequency differences of the optical and the fountain clocks are calculated. For that, a processing was introduced that combines phase and frequency data of different noise types and gaps. A respective estimator for the statistical uncertainty, based on the correlation on the data, is established. The results of both satellite-based techniques show good agreement with each other, and also clocks based on the same frequency transition agree within a 1-σ-uncertainty. The overall uncertainties obtained for TWSTFT are between 2.7e-16 and 3.5e-16 for the optical clock comparisons. Limitations for the uncertainties of the measurements are discussed in detail, the available satellite-based techniques are evaluated with respect to their advantages and drawbacks for similar measurements in the future. eng
dc.language.iso eng eng
dc.publisher Hannover : Institutionelles Repositorium der Leibniz Universität Hannover
dc.rights CC BY 3.0 DE eng
dc.rights.uri http://creativecommons.org/licenses/by/3.0/de/ eng
dc.subject frequency comparison eng
dc.subject TWSTFT eng
dc.subject optical clock eng
dc.subject Frequenzvergleich ger
dc.subject TWSTFT ger
dc.subject Optische Uhr ger
dc.subject.ddc 530 | Physik eng
dc.title Atomic clock comparisons with a 3e-16 uncertainty via geostationary satellites eng
dc.type DoctoralThesis eng
dc.type Text eng
dcterms.extent VIII, 138 S.
dc.description.version publishedVersion eng
tib.accessRights frei zug�nglich eng


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