september 2007lws 2007 halo cmes and configuration of the ambient magnetic field yang liu –...

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September 2007 LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University [email protected]

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Page 1: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Halo CMEs and Configuration of the Ambient Magnetic Field

Yang Liu – Stanford University

[email protected]

Page 2: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Introduction • Purpose: The purpose of this research is

to study influence of background field for propagation of halo CMEs.

The background field was found to have two different configurations: current sheet and non-current sheet (see, e. g. Shultz 1973; Wilcox et al. 1980; Neugebauer et al. 2002, 2004).

Current-sheet boundary

Non-current-sheet boundary

Page 3: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Current-sheet boundary

Non-current-sheet boundary

These two configurations were also successfully reproduced by Zhao & Webb (2003) based on a Potential Field Source Surface model.

Page 4: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

current-sheet boundary

Non-current-sheet boundary

Page 5: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

• 3D MHD simulation shows that type 2 and 3 CMEs are faster than type 1 (from Liu & Hayashi 2006).

• Can observation support this result?

Page 6: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Methodology• Methodology: we classify the halo CMEs by the

magnetic field computed based on the Potential Field Source Surface model, and then compare speed distributions of those three type CMEs.

• Assumption: we assume that, statistically, these three types of halo CMEs should have a similar speed distribution in the initial phase. The initial speed of a CME is suggested to be related with characteristic of the associated flare (e. g. Moon et al. 2002, Cheng et al. 2003, Zhang et al. 2004, Qiu et al. 2004).

Page 7: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Data • We looked for the halo CMEs from the CMEs

catalog of Gopalswamy’s group. 99 halo CMEs in the period from 2000 to 2004 were chosen. The solar sources were identified by that group, and were confirmed by other groups/works.

Page 8: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Examples of the three types of CMEs

Type 1 Type 2 Type 3

Page 9: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Result

Type 1 Type 2 Type 3

number 39 46 14

Percentage 39% 47% 14%

Median speed (km/s) 728 1208 1443

Mean speed (km/s) 883±403 1345±596 1530±736

Page 10: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Open: type 1

Filled: type 2 + type 3

Page 11: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Distribution of CMEs versus flare class.

Page 12: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

A correlation was found between the speed of type 3 CMEs and the peak X-ray flux of the associated flares. No such correlations are found for types 1 and 2 CMEs.

Page 13: September 2007LWS 2007 Halo CMEs and Configuration of the Ambient Magnetic Field Yang Liu – Stanford University yliu@sun.stanford.edu

September 2007 LWS 2007

Conclusions

• Types 2 & 3 CMEs appear to be significantly faster than type 1. The average speed of the former is 1388 km/s, while the latter is 883 km/s. This effect is not biased by flare importance.

• It is shown that the background magnetic configuration associated with halo CMEs does play a role in determining the speeds of the CMEs.

• A correlation was found between the speed of type 3 CMEs and the peak of X-ray flux of the associated flares.