Anomaly Detection in Geostationary Satellites

Unsupervised, Satellite-Agnostic Error Detection & Localisation

Master Thesis (2026)
Author(s)

M.C. Bak (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Contributor(s)

N. Yorke-Smith – Mentor (TU Delft - Electrical Engineering, Mathematics and Computer Science)

J.G. De Teixeira da Encarnacao – Graduation committee member (TU Delft - Aerospace Engineering)

Erwin Platen – Mentor (S&T Corporation)

Sytze Andringa – Mentor (S&T Corporation)

Faculty
Electrical Engineering, Mathematics and Computer Science
More Info
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Publication Year
2026
Language
English
Graduation Date
15-06-2026
Awarding Institution
Delft University of Technology
Programme
Computer Science
Sponsors
S&T Corporation
Faculty
Electrical Engineering, Mathematics and Computer Science
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Abstract

As Eugene Wigner showed in 1939 for the Poincaré algebra, fundamental particles can be classified using symmetry algebras. In a universe including gravity, the Poincaré algebra cannot be the correct symmetry algebra, as this is the symmetry algebra for flat space. Instead, one should consider a symmetry algebra of asymptotic symmetries, which preserve only the asymptotic structure of gravity. Many of these asymptotic symmetries are not physically useful and are therefore considered “trivial.”


In this thesis, we give a new quantum definition of trivial symmetries, namely that a symmetry is trivial if it does not change which fundamental particles are found in a classification. We then specialize to three-dimensional asymptotically Anti-de-Sitter space. To calculate which symmetries are trivial, we first determine the second cohomology group of the asymptotic symmetries. Using the second cohomology group, it is then found that the useful asymptotic symmetry algebra is given by w⊕w⊕Rw \oplus w \oplus \mathbb{R}w⊕w⊕R, where www is the Witt algebra (centerless Virasoro) algebra, whereas the standard definition of trivial symmetry gives w⊕ww \oplus ww⊕w as the useful symmetry algebra. The extra factor of R\mathbb{R}R is interpreted as a kind of center-of-mass momentum.

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