Acoustic, electromagnetic, and elastic space-time media that compute their own inverse

Journal Article (2026)
Author(s)

Dirk Jan van Manen (ETH Zürich, TU Delft - Civil Engineering & Geosciences)

Johannes Aichele (ETH Zürich)

Jonas Müller (ETH Zürich)

Marc Serra-Garcia (AMOLF Institute for Atomic and Molecular Physics)

Kees Wapenaar (TU Delft - Civil Engineering & Geosciences)

Research Group
Applied Geophysics and Petrophysics
DOI related publication
https://doi.org/10.1103/hghj-fgsw Final published version
More Info
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Publication Year
2026
Language
English
Research Group
Applied Geophysics and Petrophysics
Journal title
Physical Review Research
Issue number
3
Volume number
8
Article number
033358
Page Views
1
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Abstract

Time materials are materials with acoustic, electromagnetic, or elastic properties that change while waves are propagating through them. Waves can scatter from such temporal inhomogeneities, but due to causality, they cannot reflect back in time. As a result, time-scattered wave fields do not resemble space-scattered wave fields—which are spatially mirrored—but instead look like copies of the original signal traveling back in time. Consequently, they can form an ingredient for physical solvers of inverse problems that rely on time-reversal transformations. Here, we investigate the use of time reflections for calculating so-called focusing wave fields. We establish a one-to-one mapping between focusing wave fields and the transmitted wave fields produced by time scattering. This mapping is then used to construct a space-time medium where the time scattering anticipates the space scattering and “computes” the exact inverse transmission response for the space scattering. We demonstrate the construction with a simple numerical example of a single pulse encountering a series of time boundaries before reaching a spatial inhomogeneity. The time boundaries scatter the single pulse into a focusing wave field that subsequently focuses through the spatial inhomogeneity. With certain mild assumptions, the transmitted wave has both the same wave shape and amplitude as the original pulse, yielding a transmission coefficient of unity.