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    Electromagnetic polarization matrix and its physical interpretation

    J. J. Gil1,*,†, A. Norrman2, A. T. Friberg2, B. Fazlpour2, and T. Setälä2

    • *Contact author: ppgil@unizar.es
    • †Independent Researcher.

    Phys. Rev. A 113, 052229 – Published 26 May, 2026

    DOI: https://doi.org/10.1103/rxlq-dqjf

    Abstract

    Despite the intrinsic coupling between electric and magnetic fields in random stationary light, their polarization properties are not mutually determined. A complete second-order description thus necessitates a joint electromagnetic treatment. The 6×6 electromagnetic polarization matrix introduced here generalizes the conventional electric 3×3 matrix by incorporating both electric and magnetic contributions together with their mutual correlations. It consists of diagonal 3×3 blocks, representing the electric and magnetic polarization matrices, and off-diagonal 3×3 blocks that encode the full structure of electric-magnetic cross correlations. The information contained in this matrix can be interpreted through physically meaningful quantities such as active and reactive energy fluxes, in-phase and quadrature alignment matrices, and global indices describing electric-magnetic coupling. The formalism is applied to a field composed of two orthogonally propagating plane waves sharing a common linear electric polarization (a simple yet physically realizable configuration) that demonstrates the need for a general combined electric-magnetic representation even in free space. This approach provides a comprehensive and unified framework for characterizing electromagnetic polarization beyond the electric-field description alone, bridging classical statistical optics with quantumlike density-matrix interpretations.

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