Electron-scale dynamics of the diffusion region during symmetric magnetic reconnection in space

Reconnection in Earth's magnetotail Magnetic fields in plasmas can rapidly rearrange themselves in a process known as magnetic reconnection, which releases energy and accelerates particles. Torbert et al. used the Magnetospheric Multiscale (MMS) mission to probe a reconnection event in Earth's magnetotail—the region of plasma downstream from the planet as it moves through the solar wind. MMS has previously studied reconnection in the upstream magnetopause, but a different orbit was used to study the magnetotail, where the symmetry of the process is different. The authors measured plasma properties on scales of the electron dynamics, leading to insights that will apply in other regions where magnetic reconnection occurs. Science, this issue p. 1391 Magnetic reconnection in Earth’s magnetotail is observed on electron dynamics scales. Magnetic reconnection is an energy conversion process that occurs in many astrophysical contexts including Earth’s magnetosphere, where the process can be investigated in situ by spacecraft. On 11 July 2017, the four Magnetospheric Multiscale spacecraft encountered a reconnection site in Earth’s magnetotail, where reconnection involves symmetric inflow conditions. The electron-scale plasma measurements revealed (i) super-Alfvénic electron jets reaching 15,000 kilometers per second; (ii) electron meandering motion and acceleration by the electric field, producing multiple crescent-shaped structures in the velocity distributions; and (iii) the spatial dimensions of the electron diffusion region with an aspect ratio of 0.1 to 0.2, consistent with fast reconnection. The well-structured multiple layers of electron populations indicate that the dominant electron dynamics are mostly laminar, despite the presence of turbulence near the reconnection site.

[1]  William Daughton,et al.  Phase space structure of the electron diffusion region in reconnection with weak guide fields , 2012 .

[2]  R. P. Lepping,et al.  In situ detection of collisionless reconnection in the Earth's magnetotail , 2001, Nature.

[3]  J. Egedal,et al.  Kinetic structure of the electron diffusion region in antiparallel magnetic reconnection. , 2011, Physical review letters.

[4]  N. Bessho,et al.  Electron distribution functions in the electron diffusion region of magnetic reconnection: Physics behind the fine structures , 2014 .

[5]  S. Stammerjohn,et al.  West Antarctic Peninsula sea ice in 2005: Extreme ice compaction and ice edge retreat due to strong anomaly with respect to climate , 2008 .

[6]  David G. Sibeck,et al.  On the electron diffusion region in planar, asymmetric, systems , 2014 .

[7]  M. Fujimoto,et al.  Kinetic signatures of the region surrounding the X line in asymmetric (magnetopause) reconnection , 2016, 1602.00779.

[8]  B. Anderson,et al.  The Effect of a Guide Field on Local Energy Conversion During Asymmetric Magnetic Reconnection: Particle‐in‐Cell Simulations , 2017 .

[9]  Ritoku Horiuchi,et al.  Particle simulation study of driven magnetic reconnection in a collisionless plasma , 1994 .

[10]  J. Burch,et al.  Magnetic reconnection at the dayside magnetopause: Advances with MMS , 2016 .

[11]  Yoshitaka Saito,et al.  Construction of magnetic reconnection in the near‐Earth magnetotail with Geotail , 2011 .

[12]  M. Shay,et al.  Average properties of the magnetic reconnection ion diffusion region in the Earth's magnetotail: The 2001–2005 Cluster observations and comparison with simulations , 2009 .

[13]  A. Balogh,et al.  Cluster encounter of a magnetic reconnection diffusion region in the near‐Earth magnetotail on September 19, 2003 , 2005 .

[14]  Rumi Nakamura,et al.  Structure and dynamics of magnetic reconnection for substorm onsets with Geotail observations , 1998 .

[15]  D. Baker,et al.  Timing of magnetic reconnection initiation during a global magnetospheric substorm onset , 2002 .

[16]  R. Lysak,et al.  Cluster observations of an intense normal component of the electric field at a thin reconnecting current sheet in the tail and its role in the shock-like acceleration of the ion fluid into the separatrix region , 2005 .

[17]  Vassilis Angelopoulos,et al.  In situ evidence of electron energization in the electron diffusion region of magnetotail reconnection , 2016, 1602.08482.

[18]  K. Ogilvie,et al.  The role of upper hybrid waves in magnetic reconnection , 2003 .

[19]  J. B. Blake,et al.  Electron-scale measurements of magnetic reconnection in space , 2016, Science.

[20]  A. Vaivads,et al.  Evidence of an extended electron current sheet and its neighboring magnetic island during magnetotail reconnection , 2008 .

[21]  W. Wagner,et al.  Hydrologic resilience of the terrestrial biosphere , 2005 .

[22]  K. Glassmeier,et al.  Current sheet structure near magnetic X‐line observed by Cluster , 2003 .

[23]  R. Torbert,et al.  Spatiotemporal evolution of electron characteristics in the electron diffusion region of magnetic reconnection: Implications for acceleration and heating , 2015 .

[24]  Harry E. Petschek,et al.  Magnetic Field Annihilation , 1963 .

[25]  I. J. Rae,et al.  Tail Reconnection Triggering Substorm Onset , 2008, Science.

[26]  C. Norgren,et al.  The Physical Foundation of the Reconnection Electric Field , 2018, 1801.01090.

[27]  M. W. Dunlop,et al.  Analysis of multipoint magnetometer data , 1988 .

[28]  James Drake,et al.  Structure of the dissipation region during collisionless magnetic reconnection , 1998 .

[29]  P. Sweet 14. The neutral point theory of solar flares , 1958 .

[30]  P. Cassak,et al.  Asymmetric Magnetic Reconnection: General Theory and Collisional Simulations , 2007 .

[31]  A. Klimas,et al.  New measure of the dissipation region in collisionless magnetic reconnection. , 2011, Physical review letters.