1 solar stereoscopy - where we are and which developments do we require to progress? thomas...

43
1 Solar stereoscopy - where we are and which developments do we require to progress? mas Wiegelmann, Bernd Inhester, Feng, Judith de Patoul

Upload: helena-lester

Post on 05-Jan-2016

215 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

1

Solar stereoscopy - where we are and which developments do we require to progress?

Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

Page 2: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

2

EUV-images from2 viewpoints

3D geometry/physics of e.g. coronal loops and polar plumes

What do we have and what we want?

How?

1. Extract curve-like objects

2. Associateobjects in both

images

3. GeometricStereoscopy

4. Estimatereconstruction

error in 3D

5. Derive physical

quantities

Page 3: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

3

1. Extract curve-like objects

Processed image: A 7x7 boxcar

smoothed image was subtracted

from original

Original Trace-image(from Aschwanden,Sol. Phys. 2008)

Page 4: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

4

1. Extract curve-like objectsa) Manual loop tracing

210 manually traced loops.Trace-image, central part(Aschwanden, 2008)

Can we teach thecomputer to trace

loops automatically?

Page 5: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

5

Ridge detection

Definition of a ridge

Image intensity I (x, y) satisfies:

Inhester et al, Sol. Phys. 2008

1. Extract curve-like objectsb) Automatic loop tracing

Page 6: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

6

1. Extract curve-like objectsb) Automatic loop tracing

Page 7: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

7

Ridge location and orientation

Page 8: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

8

Interpolation of ridge positions (ridgel)

Page 9: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

9

Ridgel connection to chains

Page 10: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

10

Polynomial fits

Page 11: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

11

Merging and cleaning

Done by hand until now

Page 12: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

12

Correspondence problem: Which two loops in the two images are the projections of the same loop in the real 3D case?

solar rotation:

two viewpoints

Two-view TRACE images mimicking the EUVI image pair

(Feng et al., Sol. Phys. 2007)

2. Associate objects in both images

Page 13: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

13

Plasma outlines magnetic field lines

Can we use coronal magnetic field modelsas a proxy for 3D plasma loops?

Magnetic field and EUV-images

Page 14: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

14

Single viewpoint: SOHO/EIT, TRACEUse B-Field for feature-recognition

(Wiegelmann et al., Sol. Phys. 2005)

• Extrapolate coronal magnetic field from photosphere.

• Project 3D field lines onto an EUV-image.

• Emissivity and gradient along projected field lines.

• Alternative-1:Compare field lines and plasma.How well are they aligned?

• Alternative-2: Extract 1-D loops out of the EUV-images and compare with projections of magnetic field lines thereafter.

l

l

dsl

ds

C0

2

0

)(

||

Page 15: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

15

Linear force-free field with α=-0.01 [Mm-1]

3D-magnetic field lines, linear force-free α=-0.01 [Mm-1].Used in Marsch et. al. 2005 tostudy plasma flows with Sumer.

Alternative-1: Compare projected field lines direct with EUV-image

Page 16: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

16

Alternative-2: Compare projected field lines with extracted EUV-loops

Dotted lines:Projection of best-fit linear force-free field lines.

Loops extracted from EUVI-image with automaticfeature recognition tool.

Page 17: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

17

Can we extend this method to solve the correspondence problem of STEREO-images?

• A 3D magnetic field lines is unique.

• Project field lines onto EUVI-images[or loops extracted from EUVI].

• Measure distance of loops and projectedmagnetic field lines in both images.

• Loops close to the same field line inboth images are very likely associated.

Page 18: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

18

• Epipolar geometry reduces 3D-reconstructionproblem to several 2D problems.

• Coordinate system is defined by spacecraft locations and rotation axis of the Sun.

3. GeometricStereoscopy

From Inhester,ISSI 2006

Page 19: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

19

From Inhester,ISSI 2006

• Epipolar geometry provides necessary criteriumfor loop association: Related loops in bothimages must intersect with same epipolar lines.

• Epipolar range often not easy to specify,because ends of loops can be very faint=> Parts of loops not visible in one orboth images.

Page 20: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

20

Reconstruction ambiguity

Reconstruction of east-west orientation loops has two solutions, which one is correct?

Two-viewpoint images are not sufficient

3. GeometricStereoscopy

Page 21: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

21

4. Estimatereconstruction

error in 3D

• Features tangential to epipolar lines have highestreconstruction error.

• For east-west coronal loops this means that largest reconstruction errors occur at the loop top.

From Inhester,ISSI 2006

curve segment in-clined to epipolar line

curve segment par-rallel to epipolar line

Page 22: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

22

• 3D reconstruction error depends on the resolution w of EUVI-images and on the angle between projection planes.

• Projection angle is smaller or equal as angle between STEREO-A or B.

• For loop segments in the epipolarplane the projection angle is zeroand the error infinite.

4. Estimatereconstruction

error in 3D

From Inhester,ISSI 2006

Page 23: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

23

4. Estimatereconstruction

error in 3D

• Small separation angle between spacecraft:Association problem easy to solve,Large 3D reconstruction error.

• Large separation angle:Association problem difficult to solve,Small 3D reconstruction error.

2. Associateobjects in both

images

Page 24: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

24

Artificial STEREO-images from a model Active Region. (Wiegelmann & Inhester, Solar Phys. 2006)

Magnetic stereoscopy

Page 25: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

25

a) Original exact solution b) Pure geometric stereoscopic 3D-reconstruction.

The reconstructed 3D loops have ambiguities.

Page 26: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

26

Magnetic modeling with different models (c) potential,d) linear force-free, e) nonlinear force-free). Yellowdotted lines show the original exact loops. We used (artificial) EUV-images from two different viewpoints to constrain the magnetic loops.

Page 27: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

27

Geometric stereoscopy. We removed ambiguities (multiplesolutions) in the stereoscopic reconstruction by choosing thesolution which is closest to a given magnetic field model.(Here we used the worst model, a potential field, which was,however, sufficient to remove the ambiguities.)

Page 28: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

28

Magnetic stereoscopy Wiegelmann&Inhester 2006

Page 29: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

29

• Rigorous Test of B-field models.

• Obtain free model parameters.

• Test scaling laws.

• Get plasma parameters along loops- Temperature- Density- Pressure

Compare real + artificial images,

Loops + B-lines

Modeling,Tomography

5. Derive physical quantities

Page 30: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

30EUVI_AEUVI_B

Example-1: Active Region loops, Feng et al., ApJL 2007

NOAA 10960

Page 31: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

31

EUVI_AEUVI_B

Loops identified from unsharp mask filtered images.

1. Extract curve-like objects

Page 32: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

32

MDI : 2007-06-08T03:12:00 UT 2007-06-08T03:12:00 UT

Linear force-free extrapolation

3D magnetic field lines :

a guide to the loop correspondence

Loop correspondence

2. Associateobjects in both

images

Page 33: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

33

correspondence in the northern active region

Loop correspondence

2. Associateobjects in both

images

Page 34: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

34

Loop reconstruction

Yellow: reconstructed 3D loops

Red: best fit magnetic field lines

view from STEREO_A Northeast of AR

3. GeometricStereoscopy

Page 35: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

35

4. Estimatereconstruction

error in 3D

Yellow: Reconstructed loop with error bars.Red: Best fit linear force-free field line.

Page 36: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

36

Loop parameters

1. The linear force-free assumption is often not adequate.

2. Most of the loops cannot be approximated by planar curve segments .

3. Most of the loops are not circular.

5. Derive physicalquantities

Page 37: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

37

0 1 2 3

4

0 1 2 34

EUVI_A

EUVI_B

Example-2: Polar Plumes (Feng et al., ApJ, submitted)

1. Extract curve-like objects.Here: straight lines,intensity maximum.

2. Associateobjects in both images.

Easy for smallseparation angle.

Page 38: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

38

dotted lines: 3D reconstruction results

solid lines: extrapolations back to the solar surface.

solar limb as seen from STEREO A Side View

3. GeometricStereoscopy

4. Estimatereconstruction

error in 3D

Small separation angle: Correspondenceproblem easy to solve, no reconstruction ambiguity.But: Large 3D reconstruction error.

Page 39: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

39

Project 3D plumes onSUMER observations

(1)Doppler Shift map: No obvious outflows detected in plume regions.

(2) Ne

measured from density sensitive Si VIII line ratio

(3) Te

measured from Mg IX temperature sensitiveline pair.

5. Derive quantitiesDensity, Temperature,

Plasma flow

Page 40: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

40

• Outflow velocity along plumes is to small to make it a dominant contributor to the fast solar wind.

• 3D plumes are more horizontal than a dipole field.• Plumes are in hydrostatic equilibrium. • Temperature derived from the density scale height is

higher than electron temperature.

5. Derive quantitiesDensity, Temperature,

Plasma flow

Polar Plumes, Feng et al. 2009

Page 41: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

41

Stereoscopy vs. coronal field extrapolation

Hinode FOV

From DeRosa et al. 2009: Blue lines are stereoscopic reconstructed loops (Aschwanden et al 2008), Red lines nonlinear force-freeextrapolated field lines from Hinode/SOT.

Page 42: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

42

Stereoscopy vs. coronal field extrapolation

• Vector magnetogram data (Hinode/SOT) areessential for nonlinear force-free field modeling.

• Unfortunately Hinode-FOV covered only a smallfraction (about 10%) of area spanned by loopsreconstructed from STEREO-SECCHI images.

• Quantitative comparison was unsatisfactory.• Plan: Compare magnetic field extrapolations

from SDO/HMI and stereoscopy with STEREO/SECCHI and SDO/AIA.

• Can we combine extrapolations from photosphericmeasurements with stereoscopy?

Page 43: 1 Solar stereoscopy - where we are and which developments do we require to progress? Thomas Wiegelmann, Bernd Inhester, Li Feng, Judith de Patoul

43

Self-consistentequilibrium

Artificialimages

LOS-integration

Where to go in stereoscopy?Where to go in corona modeling?

Force-free code

SDO/HMImagnetogram

MHS code

3D Force-freemagnetic field

3D fieldlines

com

pare

Plasma along magnetic

loops

Scaling laws Tomograp

hy

Stereoscopy STEREOimages

3D EUVloops

consistent?