Evolution of Magnetic Rayleigh–Taylor Instability into the Outer Solar Corona and Low Interplanetary Space
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[1] A. Hillier. On the nature of the magnetic Rayleigh–Taylor instability in astrophysical plasma: the case of uniform magnetic field strength , 2016, 1610.08317.
[2] D. Williams,et al. FLUX CANCELLATION AND THE EVOLUTION OF THE ERUPTIVE FILAMENT OF 2011 JUNE 7 , 2016, 1606.08264.
[3] A. Srivastava,et al. Inference of magnetic field in the coronal streamer invoking kink wave motions generated by multiple EUV waves , 2016, 1606.00337.
[4] D. Williams,et al. CORONAL MAGNETIC RECONNECTION DRIVEN BY CME EXPANSION—THE 2011 JUNE 7 EVENT , 2014, 1406.3153.
[5] D. Spadaro,et al. Measurements with STEREO/COR1 data of drag forces acting on small-scale blobs falling in the intermediate corona , 2014, 1401.7984.
[6] L. van Driel-Gesztelyi,et al. INVESTIGATING THE DYNAMICS AND DENSITY EVOLUTION OF RETURNING PLASMA BLOBS FROM THE 2011 JUNE 7 ERUPTION , 2014, 1401.4824.
[7] M. L. Mays,et al. ENERGY RELEASE FROM IMPACTING PROMINENCE MATERIAL FOLLOWING THE 2011 JUNE 7 ERUPTION , 2013, 1309.1769.
[8] Pankaj Kumar,et al. Simultaneous EUV and radio observations of bidirectional plasmoids ejection during magnetic reconnection , 2013, 1307.3910.
[9] V. Petrosian,et al. PLASMOID EJECTIONS AND LOOP CONTRACTIONS IN AN ERUPTIVE M7.7 SOLAR FLARE: EVIDENCE OF PARTICLE ACCELERATION AND HEATING IN MAGNETIC RECONNECTION OUTFLOWS , 2013, 1303.3321.
[10] A. Srivastava,et al. OBSERVATIONAL EVIDENCE OF SAUSAGE-PINCH INSTABILITY IN SOLAR CORONA BY SDO/AIA , 2013, 1302.1286.
[11] L. van Driel-Gesztelyi,et al. MASS ESTIMATES OF RAPIDLY MOVING PROMINENCE MATERIAL FROM HIGH-CADENCE EUV IMAGES , 2013, 1301.4271.
[12] S. Solanki,et al. Break up of returning plasma after the 7 June 2011 filament eruption by Rayleigh-Taylor instabilities , 2012, 1202.4981.
[13] T. Berger,et al. NUMERICAL SIMULATIONS OF THE MAGNETIC RAYLEIGH–TAYLOR INSTABILITY IN THE KIPPENHAHN–SCHLÜTER PROMINENCE MODEL. I. FORMATION OF UPFLOWS , 2012 .
[14] P. Bellan,et al. Magnetic reconnection from a multiscale instability cascade , 2012, Nature.
[15] M. Luna,et al. FORMATION AND EVOLUTION OF A MULTI-THREADED SOLAR PROMINENCE , 2012 .
[16] C. R. DeVore,et al. The Effects of B/L-Dependent Heating on the Formation and Evolution of a Multi-Threaded Prominence , 2012, 1201.3559.
[17] J. Gizis,et al. DISCOVERY OF A LATE L DWARF: WISEP J060738.65+242953.4 , 2011, 1110.4351.
[18] X. Cheng,et al. INVESTIGATION OF THE FORMATION AND SEPARATION OF AN EXTREME-ULTRAVIOLET WAVE FROM THE EXPANSION OF A CORONAL MASS EJECTION , 2011, 1112.4540.
[19] K. Shibata,et al. NUMERICAL SIMULATIONS OF THE MAGNETIC RAYLEIGH–TAYLOR INSTABILITY IN THE KIPPENHAHN–SCHLÜTER PROMINENCE MODEL. II. RECONNECTION-TRIGGERED DOWNFLOWS , 2011, 1106.2613.
[20] C. Farrugia,et al. MAGNETIC KELVIN–HELMHOLTZ INSTABILITY AT THE SUN , 2011 .
[21] C. J. Wolfson,et al. The Atmospheric Imaging Assembly (AIA) on the Solar Dynamics Observatory (SDO) , 2011 .
[22] T. Berger,et al. Observation of Plasma Instabilities in Quiescent Prominences , 2010 .
[23] T. Berger,et al. QUIESCENT PROMINENCE DYNAMICS OBSERVED WITH THE HINODE SOLAR OPTICAL TELESCOPE. I. TURBULENT UPFLOW PLUMES , 2010 .
[24] A. Srivastava,et al. OBSERVATION OF KINK INSTABILITY DURING SMALL B5.0 SOLAR FLARE ON 2007 JUNE 4 , 2010, 1004.1454.
[25] P. Mein,et al. Velocity vectors of a quiescent prominence observed by Hinode/SOT and the MSDP (Meudon) , 2009, 0911.5091.
[26] J. Strutt. Scientific Papers: Investigation of the Character of the Equilibrium of an Incompressible Heavy Fluid of Variable Density , 2009 .
[27] Yukio Katsukawa,et al. Hinode SOT Observations of Solar Quiescent Prominence Dynamics , 2008 .
[28] D. Mackay,et al. Where Do Solar Filaments Form?: Consequences for Theoretical Models , 2008 .
[29] J. Stone,et al. The Magnetic Rayleigh-Taylor Instability in Three Dimensions , 2007, 0709.0452.
[30] D. Gary,et al. Magnetic Field Strength in the Solar Corona from Type II Band Splitting , 2007 .
[31] B. Inhester. Stereoscopy basics for the STEREO mission , 2006, astro-ph/0612649.
[32] T. Yokoyama,et al. Three-Dimensional Simulation of Solar Emerging Flux Using the Earth Simulator I. Magnetic Rayleigh-Taylor Instability at the Top of the Emerging Flux as the Origin of Filamentary Structure , 2006 .
[33] T. Török,et al. Confined and Ejective Eruptions of Kink-unstable Flux Ropes , 2005, astro-ph/0507662.
[34] Takaaki Yokoyama,et al. Filamentary structure on the Sun from the magnetic Rayleigh–Taylor instability , 2005, Nature.
[35] C. J. Wolfson,et al. Sun Earth Connection Coronal and Heliospheric Investigation (SECCHI) , 2000, SPIE Optics + Photonics.
[36] Sara F. Martin,et al. Conditions for the Formation and Maintenance of Filaments – (Invited Review) , 1998 .
[37] E. Priest,et al. Role of Helicity in the Formation of Intermediate Filaments , 1998 .
[38] M. Norman,et al. A numerical study of Rayleigh-Taylor instability in magnetic fluids , 1995 .
[39] E. Priest. Dynamics and Structure of Quiescent Solar Prominences , 1988 .
[40] D. Youngs,et al. Numerical simulation of turbulent mixing by Rayleigh-Taylor instability , 1984 .
[41] D. Sharp. An overview of Rayleigh-Taylor instability☆ , 1984 .
[42] B. Rompolt. Doppler brightening effect in H-alpha line for opticaly thin moving prominences , 1980 .
[43] D. Rust. Magnetic Fields in Quiescent Solar Prominences. I. Observations , 1967 .
[44] S. Chandrasekhar. Hydrodynamic and Hydromagnetic Stability , 1961 .
[45] Geoffrey Ingram Taylor,et al. The formation of a blast wave by a very intense explosion. - II. The atomic explosion of 1945 , 1950, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.