Magnetic Reconnection in Plasmas
By Juhani Birn. 2002
410 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics
View Paper: https://www.semanticscholar.org/paper/eb60afd6331452073953fa4e7401f8ed9598f9f4
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In Astronomy and Astrophysics
- B. Cerutti
- L. Sironi
- Y. Lyubarsky
- L. Comisso
- M. Begelman
- Dmitri A. Uzdensky
- A. Spitkovsky
- O. Skjaeraasen
Citations in the corpus
- Multi-scale simulations of plasma with iPIC3D (2010, background): “For instance, the time scales of phenomena occurring in a magnetic confinement fusion reactor range from the icosecond period of electron oscillations (plasma and gyro periods), to the several seconds of the plasma confinement equired for self-sustained nuclear fusion [10,37,36].”
- The Sigma Problem of the Crab Pulsar Wind (2003, background): “The Harris equilibrium is well-known to be unstable to the excitation of a variety of waves in the non-relativistic case — see, for example, Daughton (1999); Biskamp (2000) .”
- General Theory of the Plasmoid Instability (2016, background): “This crucial instability, which serves as a trigger of fast reconnection, is the plasmoid instability [2], thus dubbed as it leads to the formation of plasmoids.”
- The Case for Dynamic Models of Learners' Ontologies in Physics (2008, background): “In this excerpt, the speaker explains how energy is released during magnetic reconnection (Biskamp, 1996).”
- Three-dimensional magnetic reconnection regimes: a review (2011, background): “Complementary reviews include those by Priest and Forbes (2000); Biskamp (2000); Zweibel and Yamada (2009); Yamada et al. (2010). In Section 2 we introduce some key measures and features of magnetic field structure in 3D that are crucial to understanding where and how reconnection operates in 3D, wh”
- Scaling laws of resistive magnetohydrodynamic reconnection in the high-Lundquist-number, plasmoid-unstable regime (2010, background): “[6]) For weakly collisional systems such as the solar corona, the Lundquist number is typically very large (∼ 10(12) − 10(14)) and the Sweet-Parker reconnection time scale is of the order of years, much too slow to account for fast events such as solar flares.”
- Non-thermal particle acceleration in collisionless relativistic electron-proton reconnection (2016, background): “Magnetic reconnection is a basic plasma process often leading to the violent release of magnetic energy through rapid rear- rangement of magnetic field geometry (e.g., Biskamp 2005; Zweibel & Yamada 2009; Yamada et al. 2010).”
- On the relativistic magnetic reconnection (2005, background): “This process has been intensively studied both in laboratory plasma devices and in space (see recent monographs by Biskamp (2000) and Priest & Forbes (2000)).”