Witnessing a Large-scale Slipping Magnetic Reconnection along a Dimming Channel during a Solar Flare

We report the intriguing large-scale dynamic phenomena associated with the M6.5 flare (SOL2015-06-22T18:23) in NOAA active region 12371, observed by RHESSI, Fermi, and the Atmospheric Image Assembly (AIA) and Magnetic Imager (HMI) on the Solar Dynamics Observatory (SDO). The most interesting feature of this event is a third ribbon (R3) arising in the decay phase, propagating along a dimming channel (seen in EUV passbands) toward a neighboring sunspot. The propagation of R3 occurs in the presence of hard X-ray footpoint emission and is broadly visible at temperatures from 0.6 MK to over 10 MK through the differential emission measure analysis. The coronal loops then undergo an apparent slipping motion following the same path of R3, after a ∼80 minute delay. To understand the underlying physics, we investigate the magnetic configuration and the thermal structure of the flaring region. Our results are in favor of a slipping-type reconnection followed by the thermodynamic evolution of coronal loops. In comparison with those previously reported slipping reconnection events, this one proceeds across a particularly long distance (∼60 Mm) over a long period of time (∼50 minutes) and shows two clearly distinguished phases: the propagation of the footpoint brightening driven by nonthermal particle injection and the apparent slippage of loops governed by plasma heating and subsequent cooling.

[1]  Chang Liu,et al.  High-resolution observations of flare precursors in the low solar atmosphere , 2017, Nature Astronomy.

[2]  M. Janvier Three-dimensional magnetic reconnection and its application to solar flares , 2016, Journal of Plasma Physics.

[3]  Yuming Wang,et al.  Investigating Energetic X-Shaped Flares on the Outskirts of A Solar Active Region , 2016, Scientific Reports.

[4]  J. Qiu,et al.  OBSERVATIONS OF AN X-SHAPED RIBBON FLARE IN THE SUN AND ITS THREE-DIMENSIONAL MAGNETIC RECONNECTION , 2016, 1605.01833.

[5]  S. Solanki,et al.  Slipping reconnection in a solar flare observed in high resolution with the GREGOR solar telescope , 2016, 1605.00464.

[6]  B. Wang,et al.  SLIPPING MAGNETIC RECONNECTIONS WITH MULTIPLE FLARE RIBBONS DURING AN X-CLASS SOLAR FLARE , 2016, 1604.04982.

[7]  Haimin Wang,et al.  Unprecedented Fine Structure of a Solar Flare Revealed by the 1.6 m New Solar Telescope , 2016, Scientific Reports.

[8]  Jiajia Liu,et al.  STEREOSCOPIC OBSERVATION OF SLIPPING RECONNECTION IN A DOUBLE CANDLE-FLAME-SHAPED SOLAR FLARE , 2016, 1604.01457.

[9]  M. Karlický,et al.  SLIPPING MAGNETIC RECONNECTION, CHROMOSPHERIC EVAPORATION, IMPLOSION, AND PRECURSORS IN THE 2014 SEPTEMBER 10 X1.6-CLASS SOLAR FLARE , 2016, 1603.06092.

[10]  Yan Xu,et al.  STRUCTURE, STABILITY, AND EVOLUTION OF MAGNETIC FLUX ROPES FROM THE PERSPECTIVE OF MAGNETIC TWIST , 2015, 1512.02338.

[11]  Chang Liu,et al.  A CIRCULAR-RIBBON SOLAR FLARE FOLLOWING AN ASYMMETRIC FILAMENT ERUPTION , 2015, 1509.08414.

[12]  C. Schrijver,et al.  THERMAL DIAGNOSTICS WITH THE ATMOSPHERIC IMAGING ASSEMBLY ON BOARD THE SOLAR DYNAMICS OBSERVATORY: A VALIDATED METHOD FOR DIFFERENTIAL EMISSION MEASURE INVERSIONS , 2015, 1504.03258.

[13]  Jun Zhang,et al.  QUASI-PERIODIC SLIPPING MAGNETIC RECONNECTION DURING AN X-CLASS SOLAR FLARE OBSERVED BY THE SOLAR DYNAMICS OBSERVATORY AND INTERFACE REGION IMAGING SPECTROGRAPH , 2015, 1504.01111.

[14]  I. Craig,et al.  CURRENT SINGULARITIES AT QUASI-SEPARATRIX LAYERS AND THREE-DIMENSIONAL MAGNETIC NULLS , 2014, 1410.6545.

[15]  Jun Zhang,et al.  SLIPPING MAGNETIC RECONNECTION TRIGGERING A SOLAR ERUPTION OF A TRIANGLE-SHAPED FLAG FLUX ROPE , 2014, 1407.4180.

[16]  T. Wiegelmann,et al.  QUASI-STATIC THREE-DIMENSIONAL MAGNETIC FIELD EVOLUTION IN SOLAR ACTIVE REGION NOAA 11166 ASSOCIATED WITH AN X1.5 FLARE , 2014, 1406.7823.

[17]  Haimin Wang,et al.  AN UNORTHODOX X-CLASS LONG-DURATION CONFINED FLARE , 2014, 1405.6774.

[18]  M. Karlický,et al.  SLIPPING MAGNETIC RECONNECTION DURING AN X-CLASS SOLAR FLARE OBSERVED BY SDO/AIA , 2014, 1401.7529.

[19]  Chang Liu,et al.  STUDY OF TWO SUCCESSIVE THREE-RIBBON SOLAR FLARES ON 2012 JULY 6 , 2013, 1312.6649.

[20]  Xudong Sun,et al.  On the Coordinate System of Space-Weather HMI Active Region Patches (SHARPs): A Technical Note , 2013, 1309.2392.

[21]  P. Démoulin,et al.  The standard flare model in three dimensions - III. Slip-running reconnection properties , 2013, 1305.4053.

[22]  Institute of Theoretical Astrophysics,et al.  OBSERVING CORONAL NANOFLARES IN ACTIVE REGION MOSS , 2013, 1305.1687.

[23]  N. Vilmer,et al.  X-ray and UV investigation into the magnetic connectivity of a solar flare , 2012, 1210.2916.

[24]  Chang Liu,et al.  CIRCULAR RIBBON FLARES AND HOMOLOGOUS JETS , 2012, 1207.7345.

[25]  M. Janvier,et al.  The standard flare model in three dimensions - I. Strong-to-weak shear transition in post-flare loops , 2012 .

[26]  J. Schou,et al.  Polarization Calibration of the Helioseismic and Magnetic Imager (HMI) onboard the Solar Dynamics Observatory (SDO) , 2012 .

[27]  Masaru Shibata,et al.  Coalescence of Black Hole-Neutron Star Binaries , 2011, Living reviews in relativity.

[28]  S. Masson,et al.  Interchange Slip-Running Reconnection and Sweeping SEP Beams , 2011, 1109.5678.

[29]  R. Grauer,et al.  Numerical simulation of current sheet formation in a quasiseparatrix layer using adaptive mesh refinement , 2011, 1102.3291.

[30]  V. S. Titov,et al.  MAGNETIC TOPOLOGY OF CORONAL HOLE LINKAGES , 2010, 1011.0009.

[31]  C. J. Wolfson,et al.  The Atmospheric Imaging Assembly (AIA) on the Solar Dynamics Observatory (SDO) , 2011 .

[32]  S. Masson,et al.  THE NATURE OF FLARE RIBBONS IN CORONAL NULL-POINT TOPOLOGY , 2009 .

[33]  L. Golub,et al.  Slipping Magnetic Reconnection in Coronal Loops , 2007, Science.

[34]  P. Démoulin Where will efficient energy release occur in 3-D magnetic configurations? , 2007 .

[35]  P. Démoulin,et al.  Slip-Running Reconnection in Quasi-Separatrix Layers , 2006 .

[36]  P. Démoulin Extending the concept of separatrices to QSLs for magnetic reconnection , 2006 .

[37]  P. Démoulin,et al.  Current sheet formation in quasi-separatrix layers and hyperbolic flux tubes , 2005 .

[38]  D. Longcope Topological Methods for the Analysis of Solar Magnetic Fields , 2005 .

[39]  T. Wiegelmann Optimization code with weighting function for the reconstruction of coronal magnetic fields , 2008, 0802.0124.

[40]  G. Hornig,et al.  Theory of magnetic connectivity in the solar corona , 2002 .

[41]  S. Antiochos,et al.  A Model for Solar Coronal Mass Ejections , 1998, astro-ph/9807220.

[42]  E. Priest,et al.  Three‐dimensional magnetic reconnection without null points: 2. Application to twisted flux tubes , 1996 .

[43]  E. Priest,et al.  Three‐dimensional magnetic reconnection without null points: 1. Basic theory of magnetic flipping , 1995 .

[44]  Y. Lau Magnetic nulls and topology in a class of solar flare models , 1993 .

[45]  B. Somov,et al.  Photospheric vortex flows as a cause for two-ribbon flares: A topological model , 1988 .

[46]  T. Hirayama Theoretical model of flares and prominences , 1974 .