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PAOLO PAGANO

Origin and Ion Charge State Evolution of Solar Wind Transients during 4 – 7 August 2011

  • Autori: Rodkin D.; Goryaev F.; Pagano P.; Gibb G.; Slemzin V.; Shugay Y.; Veselovsky I.; Mackay D.H.
  • Anno di pubblicazione: 2017
  • Tipologia: Articolo in rivista
  • OA Link: http://hdl.handle.net/10447/492014

Abstract

We present a study of the complex event consisting of several solar wind transients detected by the Advanced Composition Explorer (ACE) on 4 – 7 August 2011, which caused a geomagnetic storm with Dst=−110nT. The supposed coronal sources, three flares and coronal mass ejections (CMEs), occurred on 2 – 4 August 2011 in active region (AR) 11261. To investigate the solar origin and formation of these transients, we study the kinematic and thermodynamic properties of the expanding coronal structures using the Solar Dynamics Observatory/Atmospheric Imaging Assembly (SDO/AIA) EUV images and differential emission measure (DEM) diagnostics. The Helioseismic and Magnetic Imager (HMI) magnetic field maps were used as the input data for the 3D magnetohydrodynamic (MHD) model to describe the flux rope ejection (Pagano, Mackay, and Poedts, 2013b). We characterize the early phase of the flux rope ejection in the corona, where the usual three-component CME structure formed. The flux rope was ejected with a speed of about 200kms−1 to the height of 0.25R⊙. The kinematics of the modeled CME front agrees well with the Solar Terrestrial Relations Observatory (STEREO) EUV measurements. Using the results of the plasma diagnostics and MHD modeling, we calculate the ion charge ratios of carbon and oxygen as well as the mean charge state of iron ions of the 2 August 2011 CME, taking into account the processes of heating, cooling, expansion, ionization, and recombination of the moving plasma in the corona up to the frozen-in region. We estimate a probable heating rate of the CME plasma in the low corona by matching the calculated ion composition parameters of the CME with those measured in situ for the solar wind transients. We also consider the similarities and discrepancies between the results of the MHD simulation and the observations.