Formation of Magnetic Flux Ropes during Confined Flaring Well Before the Onset of a Pair of Major Coronal Mass Ejections Georgios Chintzoglou1,*, Spiros Patsourakos2, Angelos Vourlidas3 1 School 2 of Physics, Astronomy and Computational Sciences, George Mason University, USA Physics Department, Astrogeophysics Section, University of Ioannina, Ioannina, Greece 3 Applied Physics Lab, The Johns Hopkins University, Laurel, MD, USA * Supported by the NASA Earth & Space Science Fellowship (NESSF) List of Facts - AR11429 • • • • Strongest Anti-Hale’s AR of Cycle 24! Complex (quadrupolar) configuration. Extreme shear (compared to Potential B) >70 deg along Polarity Inversion Line (PIL) Schrijver logR ≈ 5.2 (strongest PIL gradient) ! List of Facts - AR11429 • • • Multiple flare episodes (M2.1 , X5.4, X1.5). Activity continued throughout AR11429’s transit AR11429 gave off two ultra-fast CMEs (>2,000 km/sec); one of the most geo-effective of Cycle 24 (Dst = -143 nT; Richardson 2013) 12h Prior to CMEs: Confined M2.1 flare w/ visible MFR signatures <- Extremely non-radial direction for each CME 5-day Evolution of AR11429 131A + BLOS Composite AIA λ 131Å T ≈10 ΜΚ HMI BLOS - + 5-day Evolution (BLOS from HMI) Soft X-Ray and EUV flux from AR11429 211 A; Base difference. NO DIMMING after confined event 1-day evolution (prior to CMEs) 131A + BLOS Composite AIA λ 131Å T ≈10 ΜΚ HMI BLOS - + From Chintzoglou et al 2015 (in print; ApJ) DEM Temperature Maps SDO/AIA Coronal Passbands DEM Analysis for M2.1 flare Differential Emission Measure (DEM) is a measure of the amount of emitting plasma along the LOS as a function of Te. Inversion allows to estimate the Temperature of the plasma (Temperature maps; method by Plowman et al 2013). VERIFIED EXISTENCE OF HOT STRUCTURE (~10MK). From Chintzoglou et al 2015 (in print; ApJ) Slow Quasi-Static Rise during M2.1 flare arcsecs STEREO EUVI B SDO/AIA 10-20 km/sec SDO/AIA STEREO EUVI B SDO/AIA Summary of Analysis • • • • • 12 hours before the eruption, a confined eruption occurred in the NE PIL During M2.1 flare Structure rises slowly (10-20km/sec), until it stops, presumably because of strong overlying flux. DEM analysis confirms that NE MFR is a very hot structure (~10 MK) While cooling (13:49 UT), we observe the existence of a structure along the NE PIL able to support cool plasma. Evidence that NE flux-rope is formed via confined flare ~12 hours prior to its CME. Analysis II • Using a model for the Coronal field to additionally support the existence of magnetic flux ropes. • Model appropriate for analysis: Non-Linear Force-Free Field (NLFFF) Extrapolation Model (Wiegelmann 2006) • We apply several tools to detect flux ropes a. field-line integration & visualization b. |J| (current) visualization c. Fractional Twist maps 3-D Flyby around the NLFFF before eruption (2012-03-06 23:48 UT) From Chintzoglou et al 2015 (submitted; ApJ) |J| cut Integrated |J| AIA 131 A Comparing Model w/ Observations Oval structure + B-field shows detached helical structures From Chintzoglou et al 2015 (in print; ApJ) Flux rope parameters from NLFFF Fractional Twist Maps The magnetic Twist of field lines is related to the magnetic helicity via the Twist, Tn,and Writhe, Wr, numbers (Berger & Field 1984): An analytical expression for Tn, is given in Berger & Prior 2006. For force-free fields: α: force-free parameter, dl: infinitesimal length of field line. Applying this analysis on a simulated Sheared Arcade (from Aschwanden 2006), the highest value obtained for Tn is 0.5 From Chintzoglou et al 2015 (submitted; ApJ) Time evolution of <α>, <Τn>, Twisted Flux From Chintzoglou et al 2015 (in print; ApJ) Summary of Analysis II • • Only a small fraction in the vicinity of the PIL exhibits significant twist (|Tn|>0.5). Flux ropes are weakly twisted and low lying. PHYSICAL CONSIDERATIONS: • The Kink Instability (KI) is not supported by these findings nor by 131 Å imaging. • Therefore we shall consider the Torus Instability (TI) for the trigger mechanism of the CMEs -> critical decay index ncrit. Decay Index vs Height Evidence for super-critical D.I. “tunnels” (n>1.5) – allowing the ejection of the MFR From Chintzoglou et al 2015 (in print; ApJ) Conclusions Anti Hale’s AR w/ two ultra-fast (>2,000km/s) CMEs Two distinct locations (PILs) of activity within the AR Confined eruption likely created a relatively high-lying FR which subsequent flux emergence + cancellation strengthened it and led to 1st CME. • MFR1 may have formed in confined flaring and MFR2 over multiple subflaring events. • CME trigger: Torus Instability; direction: path of minimum resistance. • • • Thank you • Shear evolution suggestive of MFRs prior to eruption (see Forbes & Priest 1995) Evolution of Shear • Shear builds up w/ time Note: Increase of mean shear is consistent with rise/expulsion of Flux-rope(s). Forbes & Priest (1995) showed that while the horizontal field after eruption becomes less potential, the net field above an AR can become more potential. Decay Index vs Height Evidence for DI supercritical “tunnels” (n>1.5) – allowing the ejection of the MFR From Chintzoglou et al 2015 (submitted; ApJ) Movie showing slow rise SDO/AIA STEREO B From Chintzoglou et al 2015 (submitted; ApJ)