Hybrid quantum tensor networks for aeroelastic applications
Abstract We investigate the application of hybrid quantum tensor networks to aeroelastic problems, harnessing the power of Quantum Machine Learning (QML). By combining tensor networks with variational quantum circuits, we demonstrate the potential of QML to tackle complex time series classification and regression tasks. Our results showcase the ability of hybrid quantum tensor networks to achieve high accuracy in binary classification. Furthermore, we observe promising performance in regressing discrete variables. While hyperparameter selection remains a challenge, requiring careful optimisation to unlock the full potential of these models, this work contributes significantly to the development of QML for solving intricate problems in aeroelasticity. We present an end-to-end trainable hybrid algorithm. We first encode time series into tensor networks to then utilise trainable tensor networks for dimensionality reduction, and convert the resulting tensor to a quantum circuit in the encoding step. Then, a tensor network inspired trainable variational quantum circuit is applied to solve either a classification or a multivariate or univariate regression task in the aeroelasticity domain.
Authors
- Maya Hickmann (ORCID: https://orcid.org/0000-0002-9501-4004)
- David Quero (ORCID: https://orcid.org/0000-0003-2602-4265)
- Friedhelm Schwenker (ORCID: https://orcid.org/0000-0001-5118-0812)
- Hans-Martin Rieser (ORCID: https://orcid.org/0000-0002-1921-1436)
- Pedro Alves (ORCID: https://orcid.org/0000-0001-9524-1656)
Institutions
- Universität Ulm (DE)
- Deutsches Zentrum für Luft- und Raumfahrt e. V. (DLR) (DE)
- Institut für Arbeitsschutz der Deutschen Gesetzlichen Unfallversicherung (DE)
- Technische Hochschule Ulm (DE)
Publication Details
- Journal
- Quantum Machine Intelligence
- Published
- 2025-11-10
- DOI
- https://doi.org/10.1007/s42484-025-00327-8
- Citations
- 2
- Primary Topic
- Quantum many-body systems
- Type
- article
- Field-Weighted Citation Impact
- 2.49