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Determining the optimal communication channels of arbitrary optical systems using integrated photonic processors

A Publisher Correction to this article was published on 05 December 2023

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Abstract

Modes of propagation through an optical system are generally defined as the eigensolutions of the wave equation in the system. When propagation occurs through complicated or highly scattering media, however, modes are better identified as the best orthogonal communication channels to send information between sets of input and output apertures. Here we determine the optimal bidirectional orthogonal communication channels through arbitrary and scattering optical systems using photonic processors. The processors consist of meshes of electrically tuneable Mach–Zehnder interferometers in silicon photonics. The meshes can configure themselves based on simple power maximization or minimization algorithms, without external calculations or calibration or any prior knowledge of the optical system. The identification of the communication mode channels corresponds to a singular value decomposition of the entire optical system, autonomously performed by the photonic processors. We observe crosstalk below –30 dB between the optimized channels even in the presence of distorting masks or partial obstructions. In these cases, although the beams bear little resemblance to conventional mode families, they still show orthogonality. These findings offer potential for applications in multimode optical communication systems, promising efficient channel identification, adaptability to dynamic media and robustness against environmental challenges.

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Fig. 1: Automatically finding the best orthogonal communication modes with a pair of photonic integrated processors.
Fig. 2: Orthogonal modes between arbitrary sets of optical apertures.
Fig. 3: Orthogonal modes through obstacles and scattering media.
Fig. 4: Orthogonality between data communication channels.

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Data availability

All the data supporting the findings of this study are available within this Article and its Supplementary Information. Any additional data are available from the corresponding author on reasonable request.

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The computer codes that support the plots within this paper and other findings of this study are available from the corresponding author upon reasonable request.

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Acknowledgements

S.S., G.F., M. Sampietro, M. Sorel, A.M. and F.M. acknowledge support from the European Commission under the Horizon 2020 Programme (SuperPixels, grant no. 829116). S.S., M. Sorel, A.M. and F.M. acknowledge support from the Italian National Recovery and Resilience Plan (NRRP) of NextGenerationEU, partnership on ‘Telecommunications of the Future’ (PE00000001—program ‘RESTART’, Structural Project ‘Rigoletto’ and Focused Project ‘HePIC’). D.A.B.M. acknowledges support by the Air Force Office of Scientific Research (AFOSR, grants FA9550-17-1-0002 and FA9550-21-1-0312). Part of this work was carried out at Polifab, the micro- and nanofabrication facility of Politecnico di Milano (https://www.polifab.polimi.it/). We thank C. De Vita for his support in the realization of the phase masks used in the experiments and V. Grimaldi for his support in the development of the control electronics.

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Authors and Affiliations

Authors

Contributions

M.M. and S.S. designed the photonic chips and performed the optical measurements. F.Z., G.F. and M. Sampietro developed the electronic control systems. M. Sorel contributed to the design of the photonic chip. S.S., M.M., A.M., D.A.B.M. and F.M. conceived the experiments and analysed the experimental data. S.S., D.A.B.M. and F.M. wrote the manuscript. All the authors contributed to the revision of the manuscript. F.M. supervised the project.

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Correspondence to Francesco Morichetti.

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Nature Photonics thanks Keren Bergman, Dirk Englund and the other, anonymous, reviewer(s) for their contribution to the peer review of this work.

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Extended data

Extended Data Fig. 1 Beam shapes of orthogonal modes between arbitrary sets of optical apertures.

Complete set of beam pairs (far fields \({{{\Psi }}}_{{\hat{{{{\bf{u}}}}}}_{1,2}}\) and \({{{\Phi }}}_{{\hat{{{{\bf{v}}}}}}_{1,2}}\)) measured when the number of input M / output N apertures in the source/receiving volumes are progressively reduced, a in a non-symmetric configuration (M = 9, 8, . . . , 5; N = 9), and b in a (point-)symmetric configuration (M = N = 9, 8, . . . , 5).

Extended Data Fig. 2 Coupling strength of mode pairs established between arbitrary sets of optical apertures.

Simulated coupling strengths of modes established between the source/receiving volumes when the number of input M and output N apertures are progressively reduced a in a non-symmetric configuration (M = 9, 8, . . . , 5; N = 9), and b in a (point-)symmetric configuration (M = N = 9, 8, . . . , 5). Coupling strengths are normalized to that of the first mode when M = N = 9. Experimental data are shown in Fig. 2b,c, while measured beam shapes are reported in Extended Data Fig. 1.

Extended Data Fig. 3 Orthogonal modes through obstacles and scattering media.

The full set of obstacles used in the experiments include metal obstructions arranged as a periodic pattern of a circles (and laterally shifted in b), c donuts, d crosses, and e a microscale reproduction of the Politecnico di Milano logo. The far-field beam shapes of the first two modes \({{{\Psi }}}_{{\hat{{{{\bf{u}}}}}}_{1,2}}\) providing the maximum coupling strengths and the minimum mutual cross-talk through these obstacles are shown. For each case, bar charts show the coupling strength (σij, i = j) and the mutual cross-talk (σij, i ≠ j), which are both deteriorated with the insertion of the obstacle (dashed bars, before configuration), and can be mostly recovered by optimizing the two photonic processors (solid bars, after configuration). In the experiments reported in panel f the obstacle is a phase aberrator emulated by using an SLM; the recovery of the coupling strength (σij, i = j) and the mutual cross-talk (σij, i ≠ j) is shown for 11 different example configurations of the SLM. The peak-to-peak phase shift introduced by the phase-only aberrator is 2π.

Supplementary information

Supplementary Information

Supplementary Sections 1–3, Figs. 1–4 and caption for Video 1.

Supplementary Video 1

Camera view of the measured far field of the first (mode 1; left) and second (mode 2; right) modes during the automated setting performed by the two-processor system. The experimental conditions are the ones considered in Fig. 1e. ‘Reset’ operations correspond to random settings of all the phase actuators of the two meshes, which are scrambled at each trial. To better appreciate the mode evolution, the control algorithm is intentionally slowed down and is paused at each reset. Two modes are sequentially established (search for mode 2 starts after the convergence of mode 1); however, for a better comparison, the evolution of the two modes is shown together in the video.

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SeyedinNavadeh, S., Milanizadeh, M., Zanetto, F. et al. Determining the optimal communication channels of arbitrary optical systems using integrated photonic processors. Nat. Photon. 18, 149–155 (2024). https://doi.org/10.1038/s41566-023-01330-w

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