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Time-Distance Helioseismology at Multiple Heigh...

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May 21, 2015
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Time-Distance Helioseismology at Multiple Heights in the Solar Atmosphere

Presented at the Institute for Astronomy as part of the 2nd year research talks in Spring 2015

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skgrunblatt

May 21, 2015
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Transcript

  1. Highest SNR astrophysical lab for wave physics Wave propagation in

    a complicated environment: high T, high P, gravity and magnetic fields
  2. Outline Part I: Background Relevant physics History of seismology Part

    II: Observations Motivation Instrument setup Pipeline development Part III: Methods & Results Atmospheric travel times Disk-annulus travel times Part IV: Discussion and Summary
  3. History of Helioseismology Plaskett (1916): observed fluctuations in solar surface

    Doppler velocity Hart (1954): fluctuation of solar origin Leighton (1962): periodic, 3 mHz oscillations, convective motions on supergranule scale Claverie (1979): modal structure of oscillations integrated over solar disk: global oscillation.
  4. Outline Part I: Background Relevant physics History of seismology Part

    II: Observations Motivation Instrument setup Pipeline development Part III: Methods & Results Atmospheric travel times Disk-annulus travel times Part IV: Discussion and Summary
  5. Observations 512x512 pixel images Pixel scale: 5’’/pixel 10s cadence 17

    hour data string Wavelengths of interest: K - 769.9 nm Na I D2 - 589.0 nm
  6. Outline Part I: Background Relevant physics History of seismology Part

    II: Observations Motivation Instrument setup Pipeline development Part III: Methods & Results Atmospheric travel times Disk-annulus travel times Part IV: Discussion and Summary
  7. Atmospheric signal analysis Cross-correlate sodium, potassium signals Filter for frequencies

    of interest (3 or 7 mHz: either side of νac) Na/K Cross-correlation signal
  8. Fit model to data y(t) = A2 ! p 8⇡

    exp " !2(t Tg)2 8 # cos[!(t Tp)] Gabor wavelet equation: A: amplitude ω: 2πν, ν=freq. δω: 2πδν Tg: group time of wave Tp: phase time of wave Least squares fit to data:
  9. Atmospheric mapping 3 mHz: little atmospheric propagation, except in mag.

    regions 7 mHz: atmospheric propagation suppressed by β = 1 surface causing mode conversion, reflection (magnetogram for reference)
  10. Disk-Annulus maps Resultant signal is polluted by surface gravity waves

    Some spatial similarities apparent: signals have similar structure, but must be further refined
  11. Application to future projects **Potential dispersion relation as a func.

    of field inclination angle Use 2014 data: higher resolution Incorporate MDI, Ca and He data for better correction SAFARI, giant planet seis.
  12. Summary Successfully measured atmospheric TTs at necessary precision Need more

    sophisticated filter to get subsurface TTs Implication for understanding active regions, HMI, SAFARI