SDO/HMI multi-height velocity measurements Kaori Nagashima (MPS) Collaborators: L. Gizon, A. Birch, B. Löptien, S. Danilovic, R. Cameron (MPS), S. Couvidat.

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Presentation transcript:

SDO/HMI multi-height velocity measurements Kaori Nagashima (MPS) Collaborators: L. Gizon, A. Birch, B. Löptien, S. Danilovic, R. Cameron (MPS), S. Couvidat (Stanford Univ.), B. Fleck (ESA/NASA), R. Stein (Michigan State Univ.) HELAS VI / SOHO 28 / SPACEINN Helioseismology and Göttingen Nagashima et al SoPh 1

Standard HMI Dopplergram (Couvidat et al. 2012) HMI takes filtergrams at 6 wavelengths around Fe I absorption line at 6173 Å Calculate the line shift based on the Fourier coefficients of the 6 filtergrams – + some additional calibration to make the standard Dopplergrams (i.e., pipeline products) 2 Formation ~100km above the surface (Fleck et al. 2011) Similar to the formation layer of the center of gravity of the 6 filtergrams mA HMI SDO +34.4mA mA (from line center)

To extract multi-height info, at first, we made 3 simple Dopplergrams. But it did not work well. 3 Core Wing Far-wing Deeper layer Shallower layer core, wing, far-wing Details: Nagashima et al (ASP conference series) Core is not usable if v>1.7km/s

We tried several other definitions of Dopplergrams, and found these two look good. 4 I5 I0 I4 I1 Convert the signal into the velocity: 1.Calculate the average line profile 2.Parallel-Dopplershift the average line profile 3.Calculate the Doppler signals 4.Fit to a polynomial function of the signal

5 2. Line center (for shallower layer) – Doppler velocity of the line center derived from 3 points around the minimum intensity wavelength – Calculate the parabola through the 3 points and use its apex as the line shift So, we have 1.Average-wing Dopplergrams 2.Line-center Dopplergrams 3.And Standard HMI Dopplergrams (pipeline products) Now we have 3 Dopplergrams! Are they really “multi-height”? We tried several other definitions of Dopplergrams, and found these two look good.

Are they really “multi-height” Dopplergrams? (1)  Estimate of the “formation height” using simulation datasets (STAGGER/MURaM) 6

Are they really “multi-height” Dopplergrams? (1) ⇒ Estimate of the “formation height” using simulation datasets 7

8 Sample synthetic Dopplergrams (10Mm square) HMI observation Average wing Line center Synthetic HMI Dopplergram Standard HMI Dopplergram (pipeline product) STAGGER synthetic filtergrams (reduced resolution using HMI PSF, 3.7e2km/pix) STAGGER synthetic filtergrams (with STAGGER original resolution, 48km/pix)

Estimate of the “formation height” using simulation datasets Correlation coefficients between the synthetic Doppler velocities and the velocity in the simulation box 9 Correlation coefficients Peak heights : Line center 221km Standard HMI 195 km Average wing 170 km Line center Standard HMI Average wing 26km 25km

10 Higher w/ PSF ! (with original STAGGER resolution (no HMI PSF)) Estimate of the “formation height” using simulation datasets Correlation coefficients between the synthetic Doppler velocities and the velocity in the simulation box Correlation coefficients Peak heights : Line center 144 km Standard HMI 118km Average wing 92km Line center Standard HMI Average wing 26km 25km

km/pix Estimate of the “formation height” using simulation datasets Correlation coefficients between the synthetic Doppler velocities and the velocity in the simulation box Correlation coefficients MURaM simulation data Peak heights : Line center 150 km Standard HMI 110 km Average wing 80 km Line center Standard HMI Average wing 40km 30km

The width of the correlation peak is so large. 12 STAGGER (original resolution)STAGGER (w/ HMI PSF) Wide peaks Therefore, the Dopplergram of this wavefield should have such a wide range of contribution heights. Vz auto-correlation coefficient in the wavefield

Contribution layer is higher when the resolution is low (i.e.,w/ PSF) If the formation height in the cell is higher – In the cell it is brighter than on the intergranular lane – The cell contribution is larger than the intergranular lane’s contribution? – Therefore, the contribution layer is higher? 13 a) Continuum intensity map STAGGER simulation data b) Surface vertical velocity map

Are they really “multi-height” Dopplergrams? (2)  Phase difference measurements 14

Phase difference between Doppler velocity datasets from two different height origins 15 No significant phase difference (in p- mode regime) Atmospheric gravity wave ? (e.g., Straus et al. 2008, 2009) Significant phase difference is seen. Surely they are from different height origin. HMI observation data Line center HMI Average wing a b This means…what?

Check the height difference with Response function 16 Difference 70km * Calculate at each pixel, and average over an area with 10Mm square.

Phase difference Observed data VS Simulated data (STAGGER) 17 Line center HMI Average wing a b Very weak atmospheric gravity wave feature Ridge? Cadence 60sec Cadence 45sec Atmosphere is thin? (~550km) Or difference in Radiative damping?

Phase difference (CO 5 BOLD case) Fig. 1 in Straus et al IBIS obs.COBOLD Phase difference of the velocity fields at 250km and 70km above surface They have -negative phase shift above the acoustic cutoff - Positive phase shift in the lower frequency ranges (atmospheric gravity waves) Same as STAGGER’s results Different from STAGGER’s results Upper boundary of the atmosphere: STAGGER 550km, CO 5 BOLD 900km

Power map of HMI-algorithm Dopplergram 19 HMI observationSTAGGER Solid: HMI obs. Dotted: STAGGER Line-center HMI-algorithm Average-wing In the STAGGER power map there are some power enhance in the convection regime.

So… summary of the phase difference 20

Summary We propose two Dopplergrams other than the standard HMI- algorithm Dopplergram: – line-center Dopplergram (30-40 km above the standard) – Average-wing Dopplergram (30-40 km below the standard) Angle [deg] 0 VAL (solid) MURaM (dash) STAGGER (dot) DC limb These are useful for understanding the center-to- limb variation of helioseismology observables (e.g., Zhao et al. 2012) ? Height [km] 21 For more details, see Nagashima et al SoPh “Interpreting the Helioseismic and Magnetic Imager (HMI) Multi-Height Velocity Measurements”

22

Summary We propose two Dopplergrams other than the standard HMI- algorithm Dopplergram: – line-center Dopplergram (30-40 km above the standard) – Average-wing Dopplergram (30-40 km below the standard) We can obtain velocity information from two layers separated by about a half of a scale height in the solar atmosphere from HMI observation datasets. 23 Nagashima et al SoPh “Interpreting the Helioseismic and Magnetic Imager (HMI) Multi-Height Velocity Measurements” *We limit these discussions in the Quiet Sun.

24 Doppler signal averaged over FOV SDO velocity [m/s] core Usable only within a limited range… Limited valid range due to small wavelength separation saturated…

Angle [deg] Height [km] Calculated using SPINOR code 25