Supra-arcade downflows

SADs are dark, finger-like plasma voids that are sometimes observed descending through the hot, dense plasma above bright coronal loop arcades during solar flares. They were first reported for a flare and associated coronal mass ejection that occurred on January 20, 1999, and was observed by the SXT onboard Yohkoh. SADs are sometimes referred to as “tadpoles” for their shape and have since been identified in many other events (e.g.{{Cite journal|title = Supra-arcade Downflows in Long-Duration Solar Flare Events|journal = Solar Physics|date = 2000-08-01|issn = 0038-0938|pages = 381–399|volume = 195|issue = 2|doi = 10.1023/A:1005220604894|first = D. E.|last = McKenzie|bibcode = 2000SoPh..195..381M | s2cid=119006211 }}{{Cite journal|title = SUMER spectral observations of post-flare supra-arcade inflows|journal = Solar Physics|date = 2003-11-01|issn = 0038-0938|pages = 247–265|volume = 217|issue = 2|doi = 10.1023/B:SOLA.0000006899.12788.22|first1 = D. E.|last1 = Innes|first2 = D. E.|last2 = McKenzie|first3 = Tongjiang|last3 = Wang|bibcode = 2003SoPh..217..247I |citeseerx = 10.1.1.149.5002| s2cid=16049512 }}{{Cite journal|title = Downflow Motions Associated with Impulsive Nonthermal Emissions Observed in the 2002 July 23 Solar Flare|journal = The Astrophysical Journal|date = 2004-04-10|pages = L77–L80|volume = 605|issue = 1|doi = 10.1086/420768|first1 = Ayumi|last1 = Asai|first2 = Takaaki|last2 = Yokoyama|first3 = Masumi|last3 = Shimojo|first4 = Kazunari|last4 = Shibata|bibcode = 2004ApJ...605L..77A | s2cid=121873264 |doi-access = }}{{Cite journal|title = Posteruptive phenomena in coronal mass ejections and substorms: Indicators of a universal process?|journal = Journal of Geophysical Research: Space Physics|date = 2008-09-01|issn = 2156-2202|pages = A00B02|volume = 113|issue = A9|doi = 10.1029/2008JA013049|first1 = K. K.|last1 = Reeves|first2 = T. B.|last2 = Guild|first3 = W. J.|last3 = Hughes|first4 = K. E.|last4 = Korreck|first5 = J.|last5 = Lin|first6 = J.|last6 = Raymond|first7 = S.|last7 = Savage|first8 = N. A.|last8 = Schwadron|first9 = H. E.|last9 = Spence|bibcode = 2008JGRA..113.0B02R |url = https://scholars.unh.edu/physics_facpub/208|doi-access = free}}). They tend to be most easily observed in the decay phases of long-duration flares, when sufficient plasma has accumulated above the flare arcade to make SADs visible, but they do begin earlier during the rise phase.{{Cite journal|title = The relative timing of supra-arcade downflows in solar flares|journal = Astronomy and Astrophysics|pages = 333–340|volume = 475|issue = 1|doi = 10.1051/0004-6361:20077894|first1 = J. I.|last1 = Khan|first2 = H. M.|last2 = Bain|first3 = L.|last3 = Fletcher|bibcode = 2007A&A...475..333K |year = 2007|url = http://eprints.gla.ac.uk/28352/1/28352.pdf|doi-access = free}} In addition to the SAD voids, there are related structures known as supra-arcade downflowing loops (SADLs). SADLs are retracting (shrinking) coronal loops that form as the overlying magnetic field is reconfigured during the flare. SADs and SADLs are thought to be manifestations of the same process viewed from different angles, such that SADLs are observed if the viewer's perspective is along the axis of the arcade (i.e. through the arch), while SADs are observed if the perspective is perpendicular to the arcade axis.{{Cite journal|journal = The Astrophysical Journal|date = 2011-04-01|volume = 730|issue = 2|pages = 98|doi = 10.1088/0004-637x/730/2/98|first1 = Sabrina L.|last1 = Savage|first2 = David E.|last2 = McKenzie|arxiv = 1101.1540 |bibcode = 2011ApJ...730...98S |title = Quantitative Examination of a Large Sample of Supra-Arcade Downflows in Eruptive Solar Flares| s2cid=119273860 }}{{Cite journal|journal = The Astrophysical Journal|date = 2012-03-10|volume = 747|issue = 2|pages = L40|doi = 10.1088/2041-8205/747/2/l40|first1 = Sabrina L.|last1 = Savage|first2 = David E.|last2 = McKenzie|first3 = Katharine K.|last3 = Reeves|arxiv = 1112.3088 |bibcode = 2012ApJ...747L..40S |title = Re-Interpretation of Supra-Arcade Downflows in Solar Flares| s2cid=11690638 }}

File:Supra-Arcade Downflows from SDO AIA on 2011 Oct 02.gif AIA 131 Å on 2011 Oct 2. ]]

SADs typically begin 100–200 Mm above the photosphere and descend 20–50 Mm before dissipating near the top of the flare arcade after a few minutes.{{Cite journal|journal = The Astrophysical Journal|date = 2009-06-01|pages = 1569–1577|volume = 697|issue = 2|doi = 10.1088/0004-637x/697/2/1569|first1 = D. E.|last1 = McKenzie|first2 = Sabrina L.|last2 = Savage|bibcode = 2009ApJ...697.1569M |title = Quantitative Examination of Supra-Arcade Downflows in Eruptive Solar Flares|doi-access = free}} Sunward speeds generally fall between 50 and 500 km s⁻¹ but may occasionally approach 1000 km s⁻¹.{{Cite journal|journal = The Astrophysical Journal|date = 2013-04-20|volume = 767|issue = 2|pages = 168|doi = 10.1088/0004-637x/767/2/168|first1 = Wei|last1 = Liu|first2 = Qingrong|last2 = Chen|first3 = Vahé|last3 = Petrosian|arxiv = 1303.3321 |bibcode = 2013ApJ...767..168L |title = Plasmoid Ejections and Loop Contractions in an Eruptive M7.7 Solar Flare: Evidence of Particle Acceleration and Heating in Magnetic Reconnection Outflows| s2cid=119205881 }} As they fall, the downflows decelerate at rates of 0.1 to 2 km s⁻². SADs appear dark because they are considerably less dense than the surrounding plasma, while their temperatures (100,000 to 10,000,000 K) do not differ significantly from their surroundings.{{Cite journal|journal = The Astrophysical Journal|date = 2014-05-10|volume = 786|issue = 2|pages = 95|doi = 10.1088/0004-637x/786/2/95|first1 = Will J.|last1 = Hanneman|first2 = Katharine K.|last2 = Reeves|bibcode = 2014ApJ...786...95H |title = Thermal Structure of Current Sheets and Supra-Arcade Downflows in the Solar Corona|doi-access = free}} Their cross-sectional areas range from a few million to 70 million km² (for comparison, the cross-sectional area of the Moon is 9.5 million km²).

SADs are typically observed using soft X-ray and Extreme Ultraviolet (EUV) telescopes that cover a wavelength range of roughly 10 to 1500 Angstroms (Å) and are sensitive to the high-temperature (100,000 to 10,000,000 K) coronal plasma through which the downflows move. These emissions are blocked by Earth's atmosphere, so observations are made using space observatories. The first detection was made by the Soft X-ray Telescope (SXT) onboard Yohkoh (1991–2001). Observations soon followed from the Transition Region and Coronal Explorer (TRACE, 1998–2010), an EUV imaging satellite, and the spectroscopic SUMER instrument on board the Solar and Heliospheric Observatory (SOHO, 1995–2016). More recently, studies on SADs have used data from the X-Ray Telescope (XRT) onboard Hinode (2006—present) and the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics Observatory (SDO, 2010—present). In addition to EUV and X-ray instruments, SADs may also be seen by white light coronagraphs such as the Large Angle and Spectrometric Coronagraph (LASCO) onboard SOHO,{{Cite journal|title = The Origin of Postflare Loops|journal = The Astrophysical Journal|date = 2004-12-01|pages = 1224–1231|volume = 616|issue = 2|doi = 10.1086/425126|first1 = N. R. Jr.|last1 = Sheeley|first2 = H. P.|last2 = Warren|first3 = Y.-M.|last3 = Wang|bibcode = 2004ApJ...616.1224S | s2cid=120832655 |doi-access = }} though these observations are less common.

SADs are widely accepted to be byproducts of magnetic reconnection, the physical process that drives solar flares by releasing energy stored in the Sun's magnetic field. Reconnection reconfigures the local magnetic field surrounding the flare site from a higher-energy (non-potential, stressed) state to a lower-energy (potential) state. This process is facilitated by the development of a current sheet, often preceded by or in tandem with a coronal mass ejection. As the field is being reconfigured, newly formed magnetic field lines are swept away from the reconnection site, producing outflows both toward and away from the solar surface, respectively referred to as downflows and upflows. SADs are believed to be related to reconnection downflows that perturb the hot, dense plasma that collects above flare arcades, but precisely how SADs form is uncertain and is an area of active research.

SADs were first interpreted as cross sections of magnetic flux tubes, which comprise coronal loops, that retract down due to magnetic tension after being formed at the reconnection site. This interpretation was later revised to suggest that SADs are instead wakes behind much smaller retracting loops (SADLs), rather than cross sections of the flux tubes themselves. Another possibility, also related to reconnection outflows, is that SADs arise from an instability, such as the Rayleigh-Taylor instability{{Cite journal|journal = The Astrophysical Journal|volume = 796|issue = 2|pages = L29|doi = 10.1088/2041-8205/796/2/l29|first1 = L.-J.|last1 = Guo|first2 = Y.-M.|last2 = Huang|first3 = A.|last3 = Bhattacharjee|first4 = D. E.|last4 = Innes|arxiv = 1406.3305 |bibcode = 2014ApJ...796L..29G |year = 2014|title = Rayleigh-Taylor Type Instabilities in the Reconnection Exhaust Jet as a Mechanism for Supra-Arcade Downflows in the Sun| s2cid=117149306 }} or a combination of the tearing mode and Kelvin-Helmholtz instabilities.{{Cite journal|journal = The Astrophysical Journal|volume = 807|issue = 1|pages = 6|doi = 10.1088/0004-637x/807/1/6|first1 = M.|last1 = Cécere|first2 = E.|last2 = Zurbriggen|first3 = A.|last3 = Costa|first4 = M.|last4 = Schneiter|arxiv = 1407.3298 |bibcode = 2015ApJ...807....6C |year = 2015|title = 3D MHD Simulation of Flare Supra-Arcade Downflows in a Turbulent Current Sheet Medium| s2cid=118688215 }}

{{Reflist|2}}

• [http://sprg.ssl.berkeley.edu/~tohban/wiki/index.php/Supra-Arcade_Downflows Supra-Arcade Downflows - RHESSI Wiki (berkeley.edu)]
• [http://svs.gsfc.nasa.gov/cgi-bin/details.cgi?aid=2718 NASA: Closeup of Solar 'Tadpoles' (nasa.gov)]
• [http://xrt.cfa.harvard.edu/xpow/20120210.html Hinode/XRT: Supra-Arcade Downflows Post X-Flare (cfa.harvard.edu)]
• [http://xrt.cfa.harvard.edu/xpow/20141015.html Hinode/XRT: Supra-Arcade Downflowing Loops (cfa.harvard.edu)]

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