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    Resistive relativistic magnetohydrodynamics without Ampère’s law

    Ruben Lier1,2,3,*, Akash Jain1,2,3,†, Jay Armas1,2,3,4,‡, and Oliver Porth5,§

    • 1Institute for Theoretical Physics, University of Amsterdam, 1090 GL Amsterdam, The Netherlands
    • 2Dutch Institute for Emergent Phenomena, 1090 GL Amsterdam, The Netherlands
    • 3Institute for Advanced Study, University of Amsterdam, Oude Turfmarkt 147, 1012 GC Amsterdam, The Netherlands
    • 4Niels Bohr International Academy, The Niels Bohr Institute, University of Copenhagen, Blegdamsvej 17, DK-2100 Copenhagen Ø, Denmark
    • 5Anton Pannekoek Institute, Science Park 904, 1098 XH, Amsterdam, The Netherlands

    • *Contact author: rlier@uva.nl
    • †Contact author: ajain@uva.nl
    • ‡Contact author: j.armas@uva.nl
    • §Contact author: o.j.g.porth@uva.nl

    Phys. Rev. D 112, 083059 – Published 28 October, 2025

    DOI: https://doi.org/10.1103/stvc-tzfh

    Abstract

    Resistive magnetohydrodynamics is thought to play a key role in transient high-energy astrophysical phenomena such as flares from black hole and neutron star magnetospheres. When performing numerical simulations of resistive magnetohydrodynamics, one is faced with the issue that Ampère’s law becomes stiff in the high conductivity limit which poses challenges to the numerical evolution. We show that using a description of resistive magnetohydrodynamics based on higher-form symmetry, one can perform simulations with a generalized dual Faraday tensor without having to use Ampère’s law, thereby avoiding the stiffness problem. We also explain the relation of this dual model to a traditional description of resistive magnetohydrodynamics and how causality is guaranteed by introducing second order corrections.

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