What can we learn about coronal mass ejections through spectroscopic observations

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What can we learn about coronal mass ejections through spectroscopic observations Hui Tian High Altitude Observatory, National Center for Atmospheric Research ASP research review 2011/10/ 5

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Hui Tian High Altitude Observatory, National Center for Atmospheric Research. What can we learn about coronal mass ejections through spectroscopic observations. ASP research review. 2011/10/5 . Observation of the corona. Habbal et al. 2010, ApJ. Fe X 174 Å, imager. - PowerPoint PPT Presentation

Transcript of What can we learn about coronal mass ejections through spectroscopic observations

Page 1: What can we learn about coronal mass ejections through spectroscopic observations

What can we learn about coronal mass ejections through spectroscopic observations

Hui Tian High Altitude Observatory,

National Center for Atmospheric Research

ASP research review

2011/10/5

Page 2: What can we learn about coronal mass ejections through spectroscopic observations

Observation of the coronaHabbal et al. 2010, ApJ

Fe X 174 Å, imager Fe X 6374 Å, solar eclipse

Lower corona, coronagraph Extended corona, coronagraph

SOHO LASCO-2 White lightGround &

spaceEclipseCoronagraph

UV & X-raySpace ImagerCoronagraphSpectrograph/

spectrometer

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Coronal mass ejections (CMEs)

Credit: STEREO Science Center

Occurring frequencySolar maximum: 3-5 per daySolar minimum: 1 every 3-5

days Mass: 2 × 1014-16 g Speed: 200-2000 km/s Sometimes dimmings in EUV & X-ray

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Credit: STEREO Science Center

Space weather

Credit: SwRICredit: SOHO Daily MPEG

Earth-directed CMEs are potentially dangerous to our high-tech systems

Satellite anomalies, orbit changes, health of astronauts

Disruption of GPS & other spacecraft signals, radio signals

Damage of electric power grids & pipelines

Imaging observations at the Earth orbit can not observe the evolution of Earth-directed CMEs

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EUV spectroscopy

Curdt et al. 2001, A&A

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Combine imaging & spectroscopic observations

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Line profiles in the ejecta

Two well-separated components A nearly stationary background A high-speed components (~200 km/s) representing the

emission of the ejecta Calculate the real speed: v=Sqrt(vpos

2+vlos2)

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Spectroscopic observations of coronal dimmings

Attrill et al. 2010, Sol. Phys. McIntosh, ApJ, 2009

~20 km/s Blue shift: outflows refilling the corona Enhanced line width: growth of wave amplitude

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Blueward asymmetry of line profiles in dimming regions

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Two emission components in dimming regions

Two emission components A nearly stationary background A weak high-speed (~100 km/s)

components representing outflows

Blue shift of ~ 20 km/s and enhanced line width are caused by the superposition of the two components

Only a small portion of the materials in the dimming region are flowing outward The outflow speed is around 100 km/s

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ConclusionSpectroscopic observations can provide

valuable information on the kinematics of CMEs

3-D CME evolutions can be obtained by simultaneous imaging and spectroscopic observations

The outflow speed in the dimming region is of the order of 100 km/s, not ~20 km/s