Abstract
When waves propagate through a complex medium, they undergo several scattering events. This phenomenon is detrimental to imaging, as it causes full blurring of the image. Here we describe a method for detecting, localizing and characterizing any scattering target embedded in a complex medium. We introduce a fingerprint operator that contains the specific signature of the target with respect to its environment. When applied to the recorded reflection matrix, it provides a likelihood index of the target state. This state can be the position of the target for localization purposes, its shape for characterization or any other parameter that influences its response. We demonstrate the versatility of our method by performing proof-of-concept ultrasound experiments on elastic spheres buried inside a strongly scattering granular suspension and on lesion markers, which are commonly used to monitor breast tumours, embedded in a foam mimicking soft tissue. Furthermore, we show how the fingerprint operator can be leveraged to characterize the complex medium itself by mapping the fibre architecture within muscle tissue. Our method is broadly applicable to different types of waves beyond ultrasound for which multi-element technology allows a reflection matrix to be measured.
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Data availability
The ultrasound data generated in this study are available via Zenodo at https://doi.org/10.5281/zenodo.14845779 (ref. 54).
Code availability
The code used to postprocess the ultrasound data within this paper is available via Zenodo at https://doi.org/10.5281/zenodo.14845779 (ref. 54).
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Acknowledgements
We thank Somatex Company for providing the lesion marker. We are grateful for the funding provided by the European Research Council under the European Union’s Horizon 2020 research and innovation programme (Grant Agreement No. 819261 under the REMINISCENCE project to A.A.). This project has also received funding from Labex WIFI (Laboratory of Excellence within the French Program Investments for the Future; Grant Nos ANR-10-LABX-24 and ANR-10-IDEX-0001-02 PSL* to M.F.) and from Agence Nationale de la Recherche (Grant No. ANR-22-ASTR-0020 under the AquaMat project to A.A.). L.M.R. was supported by the Austrian Science Fund (Project No. P32300-N27, WaveLand).
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A.A. and S.R. initiated the project. A.A. supervised the project. A.L.B. and X.J. designed and performed the experiments on the granular medium. A.L.B. performed the lesion marker experiment and developed the postprocessing tools for the target detection experiment. W.L. performed the muscle tissue experiment. A.G. developed the postprocessing tools for the muscle tissue experiment. A.L.B., A.G., L.M.R., S.R. and A.A. developed the concept of the fingerprint operator and performed the theoretical study. A.L.B. and A.G. prepared the figures. A.L.B., A.G. and A.A. prepared the paper. All authors discussed the results and contributed to finalizing the paper.
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A.L.B., A.G., L.M.R., W.L., X.J., M.F., A.T., S.R. and A.A. are inventors on a French patent related to this work held by SuperSonic Imagine and CNRS (no. FR2314789, filed December 2023). M.F. is cofounder of the SuperSonic Imagine company, which is commercializing one of the ultrasound platforms used in this study.
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Extended data
Extended Data Fig. 1 Elastic target signatures encoded in the reference reflection matrix.
a, The reference reflection matrix R0 is measured on the target sphere placed in water. The confocal beamforming process applied to R0 selects not only the ballistic echo of the sphere but also its reverberations resulting from multiple reflections of bulk elastic waves (depicted by red arrows) at its inner surface. b, Matrix imaging decouples the input and output focal spots51, rin and rout, to highlight the contribution of circumferential waves (depicted by a black arrow) generated by the incoming wave at a specific angle of incidence with respect to sphere surface33. c, Cross-section of the focused reflection matrix, R0,xx(y, z), in the plane y = 0 and at depth z = 21 mm showing the diagonal contribution of the ballistic echo. d, Same matrix but at depth z = 28.5 mm showing the off-diagonal contribution of circumferential waves. e, (x, z)-section of the confocal image in the plane y = 0 showing the spatio-temporal dispersion of the target echo. f, Likelihood index map γ(r) (Eq. 2) built from the fingerprint operator indicating that we can accurately locate the target inside the reference environment (the sphere surface is highlighted by a red dashed line in panels e and f). Since in this case R ≡ R0(r0), this result serves as a consistency check for the formalism.
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Supplementary Information
Supplementary Sections 1–8, Figs. 1–15 and Table 1.
Supplementary Video 1
Dynamic view of the confocal image in the bead experiment.
Supplementary Video 2
Likelihood 3D map of sphere 1 (in colour) superimposed to the confocal image (B&W) in a dynamic scenario where the target sinks inside the vibrated dense granular suspension.
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Le Ber, A., Goïcoechea, A., Rachbauer, L.M. et al. Detection and characterization of targets in complex media using fingerprint matrices. Nat. Phys. (2025). https://doi.org/10.1038/s41567-025-03016-2
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DOI: https://doi.org/10.1038/s41567-025-03016-2