Velocity Response of the Observed Explosive Events in the Lower Solar Atmosphere. I. Formation of the Flowing Cool-loop System

We observe plasma flows in cool loops using the Slit-Jaw Imager on board the Interface Region Imaging Spectrometer (IRIS). Huang et al. observed unusually broadened Si iv 1403 Å line profiles at the footpoints of such loops that were attributed to signatures of explosive events (EEs). We have chosen one such unidirectional flowing cool-loop system observed by IRIS where one of the footpoints is associated with significantly broadened Si iv line profiles. The line-profile broadening indirectly indicates the occurrence of numerous EEs below the transition region (TR), while it directly infers a large velocity enhancement/perturbation, further causing the plasma flows in the observed loop system. The observed features are implemented in a model atmosphere in which a low-lying bipolar magnetic field system is perturbed in the chromosphere by a velocity pulse with a maximum amplitude of 200 km s−1. The data-driven 2D numerical simulation shows that the plasma motions evolve in a similar manner as observed by IRIS in the form of flowing plasma filling the skeleton of a cool-loop system. We compare the spatio-temporal evolution of the cool-loop system in the framework of our model with the observations, and conclude that their formation is mostly associated with the velocity response of the transient energy release above their footpoints in the chromosphere/TR. Our observations and modeling results suggest that the velocity responses most likely associated to the EEs could be one of the main candidates for the dynamics and energetics of the flowing cool-loop systems in the lower solar atmosphere.

[1]  B. Pontieu,et al.  Fine-scale Explosive Energy Release at Sites of Prospective Magnetic Flux Cancellation in the Core of the Solar Active Region Observed by Hi-C 2.1, IRIS, and SDO , 2019, The Astrophysical Journal.

[2]  Z. Musielak,et al.  Partially Ionized Solar Atmosphere: Two-fluid Waves and Their Cutoffs , 2019, The Astrophysical Journal.

[3]  A. Srivastava,et al.  On modelling the kinematics and evolutionary properties of pressure-pulse-driven impulsive solar jets , 2019, Annales Geophysicae.

[4]  L. B. Bellot Rubio,et al.  Quiet Sun magnetic fields: an observational view , 2019, Living Reviews in Solar Physics.

[5]  A. Srivastava,et al.  Plasma Flows in the Cool Loop Systems , 2019, The Astrophysical Journal.

[6]  H. Peter,et al.  Investigating the Transition Region Explosive Events and Their Relationship to Network Jets , 2019, The Astrophysical Journal.

[7]  Z. Musielak,et al.  Confined pseudo-shocks as an energy source for the active solar corona , 2018, Nature Astronomy.

[8]  M. Carlsson,et al.  On the generation of solar spicules and Alfvénic waves , 2017, Science.

[9]  T. Ray,et al.  High-frequency torsional Alfvén waves as an energy source for coronal heating , 2017, Scientific Reports.

[10]  L. Xia,et al.  COOL TRANSITION REGION LOOPS OBSERVED BY THE INTERFACE REGION IMAGING SPECTROGRAPH , 2015, 1507.07594.

[11]  A. Srivastava,et al.  Diagnostics of a Coronal Hole and the Adjacent Quiet Sun by The Hinode/EUV Imaging Spectrometer (EIS) , 2014, 1409.1037.

[12]  L. Golub,et al.  On the prevalence of small-scale twist in the solar chromosphere and transition region , 2014, Science.

[13]  L. Golub,et al.  On the prevalence of small-scale twist in the solar chromosphere and transition region , 2014, Science.

[14]  S. Solanki,et al.  The magnetic field in the solar atmosphere , 2014, 1410.4214.

[15]  D. Innes,et al.  On the Structure and Evolution of a Polar Crown Prominence/Filament System , 2014, 1402.4989.

[16]  F. Reale Coronal Loops: Observations and Modeling of Confined Plasma , 2010, Living Reviews in Solar Physics.

[17]  L. Teriaca,et al.  Quiet Sun Explosive Events: Jets, Splashes, and Eruptions , 2012, 1210.7667.

[18]  R. Seguin,et al.  The Interface Region Imaging Spectrograph (IRIS) , 2012, 1401.2491.

[19]  R. Erdélyi,et al.  Magnetic tornadoes as energy channels into the solar corona , 2012, Nature.

[20]  J. T. Hoeksema,et al.  The Helioseismic and Magnetic Imager (HMI) Investigation for the Solar Dynamics Observatory (SDO) , 2012 .

[21]  I. Dammasch,et al.  REDSHIFTS, WIDTHS, AND RADIANCES OF SPECTRAL LINES EMITTED BY THE SOLAR TRANSITION REGION , 2011 .

[22]  P. Colella,et al.  THE PLUTO CODE FOR ADAPTIVE MESH COMPUTATIONS IN ASTROPHYSICAL FLUID DYNAMICS , 2011, 1110.0740.

[23]  S. Solanki,et al.  The quiet Sun average Doppler shift of coronal lines up to 2 MK , 2011, 1109.4493.

[24]  B. Pontieu,et al.  The Origins of Hot Plasma in the Solar Corona , 2011, Science.

[25]  P. Konkol,et al.  Numerical simulations of the attenuation of the fundamental slow magnetoacoustic standing mode in a gravitationally stratified solar coronal arcade , 2010 .

[26]  Jiansen He,et al.  UPFLOWS IN FUNNEL-LIKE LEGS OF CORONAL MAGNETIC LOOPS , 2009, 0909.0739.

[27]  P. J. Crockett,et al.  Alfvén Waves in the Lower Solar Atmosphere , 2009, Science.

[28]  W. Curdt,et al.  The redshifted network contrast of transition region emission , 2008, 0901.0808.

[29]  D. Baker,et al.  Outflows at the Edges of Active Regions: Contribution to Solar Wind Formation? , 2008 .

[30]  E. Avrett,et al.  Models of the Solar Chromosphere and Transition Region from SUMER and HRTS Observations: Formation of the Extreme-Ultraviolet Spectrum of Hydrogen, Carbon, and Oxygen , 2008 .

[31]  E. Marsch,et al.  Signature of mass supply to quiet coronal loops , 2008, 0906.3007.

[32]  Yukio Katsukawa,et al.  Chromospheric Anemone Jets as Evidence of Ubiquitous Reconnection , 2007, Science.

[33]  J. Qiu,et al.  Direct Observation of High-Speed Plasma Outflows Produced by Magnetic Reconnection in Solar Impulsive Events , 2007, 0709.2329.

[34]  A. Ferrari,et al.  PLUTO: A Numerical Code for Computational Astrophysics , 2007, astro-ph/0701854.

[35]  Study of a transient siphon flow in a cold loop , 2006 .

[36]  J. Klimchuk On Solving the Coronal Heating Problem , 2005, astro-ph/0511841.

[37]  D. Banerjee,et al.  Transition region small-scale dynamics as seen by SUMER on SOHO , 2004 .

[38]  R. Erdélyi,et al.  Solar chromospheric spicules from the leakage of photospheric oscillations and flows , 2004, Nature.

[39]  D. Müller,et al.  Dynamics of solar coronal loops I. Condensation in cool loops and its effect on transition region lines , 2003 .

[40]  D. Banerjee,et al.  An EUV Bright Point as seen by SUMER, CDS, MDI and EIT on-board SoHO , 2003 .

[41]  Antonino Francesco Lanza,et al.  A Transient Heating Model for Coronal Structure and Dynamics , 2003 .

[42]  J. G. Doyle,et al.  Temporal variability in the Doppler-shift of solar transition region lines , 2002 .

[43]  H. Peter The Chromosphere in Coronal Holes and the Quiet-Sun Network: An He I (584 Å) Full-Disk Scan by SUMER/SOHO , 1999 .

[44]  J. Dowdy Observational evidence for hotter transition region loops within the supergranular network , 1993 .

[45]  V. Hansteen A new interpretation of the redshift observed in optically thin transition region lines , 1993 .