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Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development of two magneto- hydrostatic coronal models for modeling large-scale coronal and heliospheric magnetic fields (WSO, MDI, HMI). III. Prediction of disturbances in the corona and heliosphere (CISM, WSO, MDI, HMI). (See sun.stanford.edu/~xuepu/PUBLICATION/ for details of 118 papers)

My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

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Page 1: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

My 20 Years of Service at Stanford Solar Physics Group

I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI).

II. Development of two magneto-hydrostatic coronal models for modeling large-scale coronal and heliospheric magnetic fields (WSO, MDI, HMI).

III. Prediction of disturbances in the corona and heliosphere (CISM, WSO, MDI, HMI).

(See sun.stanford.edu/~xuepu/PUBLICATION/ for details of 118 papers)

Page 2: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

I. Improvement of synoptic maps of the photospheric magnetic fieldI.1 The uniqueness of the PFSS model

solution (Zhao & Hoeksema, 1993).I.2 The “Synoptic frame” (Zhao et al.,

1996; ...).I.3 The “Synchronic frame" (Zhao et al.,

2010; …).

Page 3: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

II. Development of two magneto-hydrostatic coronal models

II.1 The HCCSSS model (Zhao & Hoeksema, 1994; …): The latitude-independence of Br, The radial variation of HCS, The north-south displacement of HCS, Define and identify the base of the heliosphere.II.2 The non-force-free helical coronal magnetic field

model (Zhao and Hoeksema, 2000; …).

Page 4: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

III. Prediction of the disturbances in corona and heliosphere

III.1 Relationship among IMF Bs events, the orientation of magnetic clouds, the orientation of post-eruption X-ray arcades, and the local inclination of the HCS

(Zhao & Hoeksema, 1998, ...).III.2 The circular (Zhao et al., 2002; …) & elliptic

cone models (Zhao, 2005; 2008, …).III.3 New algorithm for inverting 3-D direction

(Zhao, 2011).

Page 5: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

III.4 Predict ICME arrival time at Earth using cone model parameters (Odstrcil, Riley & Zhao, 2004; ...).

III.5 Model two kinds of coronal closed regions and two kinds of boundary layers between coronal holes (Zhao & Webb, 2003).

III.6 Predict the existence of the interaction between fast stream and slow CME based on observation of shock pairs ( Zhao, 1992).

Page 6: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development
Page 7: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

The 2010.08.01 Wide CME and its Trigger: A New Cause of

Sympathetic Coronal Activities

The solar group meeting, 2011.05.20

Page 8: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

1. The 20100801 ``global solar storm’’

Schrijver and Title (2010) identified a "global solar storm“ on 2010.08.01.

Page 9: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

Partial-haloN37W32 07:50UT

Full-haloN13E2108:26UT

Figure 1. The sources of partial- and full-halo CMEs from the 20100801 USAF/NOAA Report .

Page 10: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

CMEs must originate in coronal closed field regions since CMEs are generated by free magnetic energies.

The angular width of CMEs are often associated with the angular width of their source closed region.

To understand the cause of formation, we need to first quantitatively estimate the spatial size of the full halo CME or the global solar storm, then find out the CME source region, and finally figure out the possible trigger.

Page 11: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

2. The wide angular width of the 2010.08.01 full-halo CME

• The apparent angular width of limb CMEs approximately represents the true angular width of CMEs. The upper limit of the limb CME width is ~110° (Burkepile et al., 2004).

• To estimate the spatial size of the event, we need to find out the limb CME that corresponds to the 20100801 SOHO full-halo CME.

Page 12: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

Fig 2 The full (left) and partial (right) halo CMEs and their elliptic outlines identified using 5-point method (the five green dots in the two panels).

SOHO C3

Combining the elliptic outline and our ZEC model we can find out thepropagation direction of the full halo CMEs to be N25E09.

STEREO A (B) was located at the longitude of W78.4 (E71.2 ) from the Earth. Thus STEREO A (B) would observe an east limb CME (a west partial halo CME). That is why CACTUS code did not work for the west CME.

Page 13: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

Figure 3. The difference images of COR2 (from CACTUS web page) show that the angular width of the east limb CME is 144°, as shown by the two dashed white lines.

The CACTUS code is good for Identifying limb CME. Its fail in the west CMESuggests that it is a partial halo CME, instead of a limb CME.

Behind Ahead

Page 14: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

3. A narrow east limb CME preceding the wide east limb COM

Fig. 4 The COR2 images observed by STEREO Ahead and Behind between 08:24:00 and 10:24:00. It shows a narrow east limb CMEpreceding the east wide limb CME

Behind Ahead

Page 15: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

The COR2 movie shows that the wide CMEs follow a narrow (50°) limb CME.

Page 16: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

4. The trigger of the 2010.08.01 wide CME & global solar storm

Two possible causes have been suggested in literature forthe sympathetic flares: (1) propagation of impulse signal excited by one coronal activity along magnetic field linesjoining related regions to other(s), (2) simultaneouslychanges of magnetic field in related wide-separated sourceregions. The fact that the wide separation of source regionsand small difference of onset times rejects the first cause

because it is impossible for signal carrier like waves andcorpuscular flow to propagate so fast!

Page 17: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

4.1 The global changes of the photospheric magnetic field

The arc-second resolution and 45-second candence HMI magnetograms make it possible to examine the global change of the photospheric magnetic field between 05:00:00 and 07:30:00. If the global change is the cause, the change must be rapid to generate coronal activities, and may be manifested in feature’s location, size and

field strength.

Page 18: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

The movie of 45s HMI ls images between 05:00:00 and 07:30:00. No significant global time variation in shape & size!

Page 19: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

The movie of difference images from the first 0500 image between 0500 & 0730. No siginificant emerging in 2.5 hours.

Page 20: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

The movie of fifference images in time interval of 12 min.No significant global change in field strength. The global change of field should also not be the cause!!!

Page 21: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

4.2 Large closed region and Global CME trigger

• CMEs must originate in coronal closed field regions since, and all coronal closed regions are sandwiched by coronal holes (Zhao & Webb, 2003).

• Based on observed coronal holes and the location of the partial- and full-halo CMEs,

we can determine the coronal closed region that contains all associated coronal activities.

Page 22: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

Fig. 5 The open (coronal hole, H) and closed (bright) regions shown in AIA 193 and EIT 195 images. The HMI & WSO magnetograms show the thick polarity-inversion lines(PIL). The AIA dark regions along PILs are not coronal holes.

N37W32

N20E35

AIA 193 08.01_23

HMI 08.01_23

WSO 08.01_18EIT 195 08.01_00

H

H

H HH

H

Page 23: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

2010-08-01 23:00

2010-08-05 23:00 2010-07-19 23:00 2010-0725 23:00

Figure 6 The whole-surface distribution of observed coronal holes. The wide closed region between two identified holes is the source region of the global storm. Its angular width is similar to the wide CME.

H

H

H

Page 24: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

The wide closed field region contains a few BMRs. The outmost closed field lines of the wide closed region confine all underlying BMRs.

Schrijver and Title (2010) have shown that the source of various coronal activities are physically related through magnetic linkage, and all coronal activities are connected by "magnetic faults", i.e., separatrices, separators, and quasi-separatrix layers. The magnetic faults before onset of the acticities are in metastable configuration where small changes in surrounding plasma currents can set off big electromagnetic storms.

Page 25: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

As shown in the AIA movie and EUVI movie, firstly a filament near the north polar hole expand upward, then erupt, and finally all magnetic arcades at different BMRs expand and erupt simultaneously. It appears that this filament eruption opened up the outermost closed magnetic field lines of the wide closed field region that originally confine all metastable structures through magnetic stress, and the loss of the stress makes those metastable structures becoming unstable or loss of equilibrium all at once, i.e., triggers the wide Earth-directed CME or the global solar storm.

Page 26: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

5. Summary and Discussion

5.1 We show that the angular width of the full halo CME or the global solar storm on 2010.08.01 is ~140°, significantly wider than the upper angular-width limit of CMEs. This wide angular width can be estimated from corresponding limb CMEs, and

provide a way to define the global solar storm. 5.2 Before the onset of the global solar storm, the

high-cadence HMI images do not show any rapid global change of the photospheric magnetic features in their shape, size and field stregth.

Page 27: My 20 Years of Service at Stanford Solar Physics Group I. Improvement of inner boundary condition for data-based coronal models (WSO, MDI, HMI). II. Development

5.3 We show that the 2010.08.01 wide CME occurs in a very wide coronal closed f region and that the closed region contains a few metastable BMRs confined by its outmost magnetic field lines. The open-up of the outmost magnetic field lines by the filament eruption within the closed region makes all underlying metastable structures to be unstable.This is the trigger of the 2010.08.01 wide CMEand global solar storm. It may also be the cause of other sympathetic coronal activities.