台灣清華大學, 物理系 helioseismology (ii) global and local helioseismology (2010.08,...

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台台台台台台台台台 Helioseismology (II) Global and Local Helioseismology (2010.08, 台台 ) 台台Dean-Yi Chou

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Page 1: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

台灣清華大學, 物理系

Helioseismology (II)

Global and Local Helioseismology

(2010.08, 北京 )

周定一 Dean-Yi Chou

Page 2: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Helioseismolgy

Using solar p-mode oscillations (waves) measured on the solar surface to probe the solar interior.

Page 3: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Basic Principle to probe Solar Interiors

Different modes penetrate into different depths.

Page 4: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Observations in Helioseismology

Using solar p-mode oscillations (waves) measured on the solar surface to probe the solar interior.

Observations set r = R

But it still gives the same dispersion relation:

Page 5: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Local Helioseismolgy

Using solar p modes measured on the solar surface to probe the local properties of the solar interior.

Global Helioseismolgy

Using solar p modes measured on the solar surface to probe the global properties of the solar interior.

The life time of p modes used in global helioseismology needs to be long enough to go around the Sun.

This gives a criterion: l < 150

It needs higher l (shorter wavelength).

Page 6: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Examples of Important Achievements in Global Helioseismology

• Confirm and refine the standard model

• Depth dependence of sound speed

• Differential rotation pattern

• Wave excitation mechanism

• Solar-cycle variations of rotation and sound speed near the base of the convection zone ???

Page 7: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Observations in Helioseismology

Using solar p-mode oscillations (waves) measured on the solar surface to probe the solar interior.

Observations set r = R

But it still gives the same dispersion relation:

Page 8: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

k-ω Diagram

Page 9: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Sound Speed and Density Profile

Page 10: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Internal Differential Rotation

Page 11: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Internal Differential Rotation

(comparison of different methods)

Page 12: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Local Helioseismolgy

Using solar p-mode oscillations measured on the solar surface to probe the local properties of the solar interior.

Local properties (local inhomegeneity):

1. magnetic fields

2. flows

3. thermal perturbation

4. other local properties

Page 13: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

> Fourier-Hankel decomposition (Braun et al. 1987)> Ring-diagram Analysis (Hill 1988)> Time-Distance Analysis (Duvall et al. 1993)> Acoustic Imaging (Chang et al. 1997)> Holography ? (Chou et al. 2007)> Direction Filter (Chou et al. 2009)

Techniques in Local Helioseismology

Page 14: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Examples of Important Achievements in Local Helioseismology

• Flows around sunspots

• Flows in the convection zone (near surface)

• Sound-speed perturbation around sunspots

• Meridional flows in the convection zone (distribution and solar-cycle variations)

• Acoustic power in sunspots

Page 15: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Ring-diagram Analysis (Hill 1988)

Basic principle:

1. Flows affect p-mode frequencies.

2. 2-d flow patterns can be derived from frequency shifts.

Page 16: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 17: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 18: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 19: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

The average velocity over the region, (Ux, Uy), is determined by fitting power spectra to

It needs inversion to obtain depth distribution.

Page 20: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Flow pattern from ring-diagram analysis

d = 7.1 Mm

Page 21: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Time-Distance Analysis (Duvall et al. 1993)

Measuring changes in travel time due to inhomogeneity

Cross-correlation functions1

2

Page 22: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 23: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Fit cross-correlation functions to a Gabor wavelet

Page 24: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Information from travel time

flow velocity

wave speed perturbation

Through inversion, the distributions of flow velocity and wave speed perturbation below the surface can be obtained.

Page 25: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Time-Distance Analysis (Duvall et al. 1993)

Measuring changes in travel time due to inhomogeneity

Cross-correlation functions1

2

Page 26: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Kosovichev et al. (2000) (MDI data)

flow velocity and wave-speed perturbation in an active region

from time-distance analysis

16 Mm

Page 27: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

wave-speed perturbation for an active region

Kosovichev et al. (2000) (MDI data)

Page 28: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Kosovichev et al. (2000) (MDI data)

wave-speed perturbation for an emerging flux region

8 hour interval

1

2

3

Page 29: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Acoustic Imaging (Chang et al., 1997)

Is it possible to image the solar interior with acoustic waves measured on the surface?

Page 30: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

imaging = adding signals in phase

Principle of imaging

There is no such a lens for the solar interior.

One needs a computational lens.

Page 31: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 32: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 33: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Constructed Images from Acoustic Imaging

Page 34: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Although the computation lens is focused on the target point, information along the ray path is contained in the signals used in reconstruction.

The phase and intensity information at a target point include information along the ray path.

One needs to do inversion to obtain more precise distribution of inhomogeneity.

Page 35: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou
Page 36: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Sound-speed perturbation from inversion of travel-time perturbation in acoustic imaging

vertical cut

measured inversion

measured inversion

(Sun & Chou, 2001)

54Mm

169 Mm

Page 37: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Acoustic imaging technique has been used to map the far side of the Sun.

Application:

Page 38: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

Limits of local helioseimology

> Modes of longer wavelength penetrate deeper.

> β increases with depth rapidly.

1. Limit on spatial resolution

2. Limit on depth

Page 39: 台灣清華大學, 物理系 Helioseismology (II) Global and Local Helioseismology (2010.08, 北京 ) 周定一 Dean-Yi Chou

The EndThe End