Magnetic reconnection is a process where magnetic field lines break and reconnect, releasing energy and observed in phenomena like coronal mass ejections.Magnetic reconnection is a process in a conductive plasma, in which the magnetic field lines rearrange, changing their topology. In plasma, charged particles are usually 'frozen' to the field lines (the frozen-in condition). However, in thin current sheets where oppositely directed fields meet, the frozen-in condition breaks down: the lines tear and reconnect, converting magnetic field energy into kinetic energy of plasma jets and heat. This is the primary mechanism powering solar flares and substorms in planetary magnetospheres.
The key idea of breaking and reconnecting magnetic field lines in current sheets to explain solar flares was proposed by James Dungey in 1953. Later, in 1957–58, Peter Sweet and Eugene Parker independently developed a quantitative model of steady-state reconnection (the Sweet–Parker model), which, however, predicted energy release that was too slow. The problem of fast reconnection stimulated the development of new models in the 1990s: Biskamp included the Hall effect, and work by Shay and Drake showed that charge separation in the ion-inertial region dramatically accelerates the process. Modern space missions (Cluster, MMS) and laboratory experiments (MRX, SPHEX) have confirmed the importance of kinetic effects.
In plasma, described by the equations of magnetohydrodynamics, the magnetic field is frozen into the medium, and its topology is preserved if the conductivity is infinite. When plasma volumes with antiparallel fields converge, a thin current sheet forms at the boundary, where the current density sharply increases and the magnetic field weakens. Due to finite resistivity or kinetic effects such as electron inertia and charge separation (the Hall term in the generalized Ohm's law), the frozen-in condition breaks down. Then the field lines reconnect, and magnetic energy dissipates. In fast regimes (e.g., Hall reconnection), the process rate is determined by the Alfvén time and depends only weakly on conductivity. Particle acceleration occurs as a result of the direct action of the electric field associated with the changing magnetic flux, and through stochastic processes in turbulent magnetic structures. Reconnection is often accompanied by the formation of narrow plasma jets heated to millions of degrees.
This process is responsible for solar flares that can disrupt radio communications and damage satellites, as well as for auroras. In fusion reactors, controlling reconnection is necessary for plasma confinement.
A single magnetic reconnection event on the Sun can release as much energy in a few minutes as humanity consumes over hundreds of thousands of years.
| m_phys | variable | physical (renormalized) mass — mass kilogram |
| m_0 | variable | bare (Lagrangian) mass — mass kilogram |
| Z | variable | field strength renormalization constant |
| H_{\text{HFI}} | variable | magnetic hyperfine interaction Hamiltonian — hamiltonian joule |
| \boldsymbol{\mu}_I | variable | nuclear magnetic moment — magnetic moment ampere square metre |
| \mathbf{A} | variable | hyperfine coupling tensor — tensor joule per ampere square metre |
| \mathbf{S} | variable | electron spin operator — spin operator |
| \cdot | operator | scalar product of vectors — dot product |













