1 / 22

Pulsations and magnetic activity in the IR

Pulsations and magnetic activity in the IR. Rafa Garrido & Pedro J. Amado Instituto de Astrofísica de Andalucía, CSIC. Granada. Acoustic oscillations. Angular dependence (l,m). Radial dependence (n). 1996 standard solar model. inclusion of He settling

Télécharger la présentation

Pulsations and magnetic activity in the IR

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Pulsations and magnetic activity in the IR Rafa Garrido & Pedro J. Amado Instituto de Astrofísica de Andalucía, CSIC. Granada

  2. Acoustic oscillations Angular dependence (l,m) Radial dependence (n)

  3. 1996 standard solar model inclusion of He settling & improved physics base of convection zone better physics for core needed Standard solar model

  4. Standard solar model Differential rotation

  5. Small and large separations Solar oscillations (VIRGO-SOHO)

  6. Asteroseismic diagram:J. C. Christensen-Daslgaard, Rev. Mod. Phys., 74, 1073

  7. d Scuti g Doradus Variability Zoo

  8. Giants  UMa  Hya GSC 09137- 03505  aBoo 

  9. LAST RESULTS WITH HARPSB. Mosser (Corot week 6: May 2004, Orsay) • A clear signature of the large separation : • Dn  89 mHz

  10. HARPS PERFORMANCE 2 minutes integration time for V=6 on the ESO 3.6m: σv=1 ms-1@ vsini= 0 kms-1 σv=3 ms-1@ vsini=10 kms-1

  11. Benefits from the IR Flux gain

  12. Benefits from the IR magnetic sensitivity

  13. Problems • Theory • mode selection (amplitudes) • amplitude & phase changes • input physics in models • convection & overshooting • diffusion & settling • rotation • magnetic field • Observations • mode identification (spectroscopy & photometry) • data analysis

  14. Active stars:Science goals • Dynamo geometry • Solar-like or something different? • Polar spots and active belts • Spot structure • Resolved or not? • Differential rotation and meridional flows • Lifetimes of individual spots and active regions • Stellar “butterfly diagrams” • Different stellar types • Pre-main sequence stars • Young main-sequence stars with[out] radiative interiors • Subgiants and giants

  15. A A Intensity Intensity -v sin i v(spot) v sin i -v sin i v(spot) v sin i Doppler Imaging

  16. Data requirements • Time-series of hi-res (R > 30000) spectra: • Good supply of unblended intermediate-strength lines (!) • Broad-band light-curves. • TiO and other temperature diagnostics.

  17. Least-Square Deconvolution • Assume observed spectrum = mean profile convolved with depth-weighted line pattern: • De-convolve mean profile zkvia least squares: • S/N improves from ~100 to ~2500 per 3 km s–1 pixel with ~2500 lines. Depth-weighted line pattern,  - KNOWN  Mean profile, z (UNKNOWN) Rotationally broadened spectrum, r – KNOWN =

  18. DI Maps AB Dor

  19. DI Maps VW Cep

  20. ZDI Maps AB Dor

  21. Benefits from the IR • Spectral lines are less blended in the infrared. Hence, line profile variations are more clearly detected • The Zeeman effect is enhanced for lines in the IR • Radiation flux and pulsation amplitudes increase with increasing wavelength for cooler stars. • IR lines can probe different parts of the atmosphere.

  22. Benefits from the IR • Sun continuum contrast between photosphere and Tspot =4250 K: • ≈ 20% @ 0.6 µm • ≈ 70% @ 2.2 µm • Resolving the telluric absorption lines (intrinsically narrow ~5 km s−1) Pontoppidan & van Dishoeck, 2004, astroph 0405629 • Zeeman sensitivity: the Fe I line at 1.56 µm splits by twice the FWHM in 1.5 kG fields (slowly rotating stars): 2-3 times more sensitive than optical lines (Giampapa PASP 109)

More Related