Abstract
The dynamics of cold strongly magnetized plasma -- traditionally the domain of force-free electrodynamics -- has recently been reformulated in terms of symmetries and effective field theory, where the degrees of freedom are the momentum and magnetic flux carried by a fluid of cold strings. In physical applications where the electron mass can be neglected one might expect the presence of extra light charged modes -- electrons in the lowest Landau level -- propagating parallel to the magnetic field lines. We construct an effective description of such electric charges, describing their interaction with plasma degrees of freedom in terms of a new collective mode that can be thought of as a bosonization of the electric charge density along each field line. In this framework QED phenomena such as charged pair production and the axial anomaly are described at the classical level. Formally, our construction corresponds to gauging a particular part of the higher form symmetry associated with magnetic flux conservation. We study some simple applications of our effective theory, showing that the scattering of magnetosonic modes generically creates particles and that the rotating Michel monopole is now surrounded by a cloud of electric charge.
Highlights
IntroductionDiverse sets of physical phenomena across vastly different length scales are controlled by the dynamics of magnetic fields in plasma
A particular regime of a strongly magnetized plasma is obtained when one considers a situation where electric charges are sufficiently plentiful as to screen the electric field to zero, but sufficiently diffuse in that one can ignore their collective stress-energy. Such a regime is conventionally described by the equations of force-free electrodynamics (FFE), which describes the non-linear dynamics of magnetic field lines at zero temperature [2–4]
Note that the bosonic field φ provides an alternative description of the dynamics of the charge sector, which may be more convenient for certain purposes
Summary
Diverse sets of physical phenomena across vastly different length scales are controlled by the dynamics of magnetic fields in plasma. A particular regime of a strongly magnetized plasma is obtained when one considers a situation where electric charges are sufficiently plentiful as to screen the electric field to zero, but sufficiently diffuse in that one can ignore their collective stress-energy Such a regime is conventionally described by the equations of force-free electrodynamics (FFE), which describes the non-linear dynamics of magnetic field lines at zero temperature [2–4]. This theory has no preferred rest frame.
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